Wednesday, December 19, 2012

Binaural beats by Wiki(updated April 2016)

A binaural beat is an auditory illusion perceived when two different pure-tone sine waves, both with frequencies lower than 1500 Hz, with less than a 40 Hz difference between them, are presented to a listener dichotically, that is one through each ear.[1] For example, if a 530 Hz pure tone is presented to a subject's right ear, while a 520 Hz pure tone is presented to the subject's left ear, the listener will perceive the auditory illusion of a third tone, in addition to the two pure-tones presented to each ear. The third sound is called a binaural beat, and in this example would have a perceived pitch correlating to a frequency of 10 Hz, that being the difference between the 530 Hz and 520 Hz pure tones presented to each ear.[2]

 

Contents

 

History


The term 'binaural' literally signifies 'to hear with two ears', and was introduced in 1859 to signify the practice of listening to the same sound through both ears, or to two discrete sounds, one through each ear. It was not until 1916 that Carl Stumpf (1848-1936), a German philosopher and psychologist, distinguished between dichotic listening, which refers to the stimulation of each ear with a different stimulus, and diotic listening, the simultaneous stimulation of both ears with the same stimulus.[3][4]

Later, it would be become apparent that binaural hearing, whether dichotic or diotic, is the means by which the geolocation and direction of a sound is determined.[5][6]

Scientific consideration of binaural hearing began before the phenomenon was so named, with the ideas articulated in 1792 by William Charles Wells (1757–1817), a Scottish-American printer, and physician at Saint Thomas' Hospital, London. Wells sought to theoretically examine and explain aspects of human hearing, including the way in which listening with two ears rather than one might affect the perception of sound, which proceeded from his research into binocular vision.[7][8]

Subsequently, between 1796 and 1802, Giovanni Battista Venturi (1746 - 1822), an Italian physicist, savant, man of letters, diplomat, and historian of science, conducted and described a series of experiments intended to elucidate the nature of binaural hearing.[9][10][11][12] It was in an appendix to a monograph on color that Venturi described experiments on auditory localization using one or two ears, concluding that "the inequality of the two impressions, which are perceived at the same time by both ears, determines the correct direction of the sound."[13][14]

However, none of Venturi's contemporaries at the end of the eighteenth and beginning of the nineteenth centuries considered his original work worthy of citation or attention, with the exception of Ernst Florens Friedrich Chladni (1756–1827), a German physicist and musician, who is widely cited as the father of acoustics. After investigating the behavior of vibrating strings and plates, and examining the way in which sound appeared to be perceived, Chladni acknowledged Venturi's work, agreeing with him that the ability to determine the location, and direction of sound depended upon detected differences in a sound between both ears, including amplitude and frequency, subsequently denoted by the term 'interaural differences'.[15][16][17]

Other significant historic investigations into binaural hearing include those of Charles Wheatstone (1802–1875), an English scientist, whose many inventions included the concertina and the stereoscope, Ernst Heinrich Weber (1795–1878), a German physician cited as one of the founders of experimental psychology; and August Seebeck (1805–1849), a scientist at the Technische Universität, Dresden, remembered for his work on sound and hearing. Like Wells, these researchers attempted to compare and contrast what would become known as binaural hearing with the principles of binocular integration generally, and binocular color mixing specifically. They found that binocular vision did not follow the laws of combination of colors from different bands of the spectrum. Rather, it was found that when presenting a different color to each eye, they did not combine, but often competed for perceptual attention.[18][19][20][21]

Meanwhile, of Wheatstone conducted experiments in which he presented a different tuning fork to each ear, stating:

It is well known, that when two consonant sounds are heard together, a third sound results from the coincidences of their vibrations; and that this third sound, which is called the grave harmonic, is always equal to unity, when the two primitive sounds are represented by the lowest integral numbers. This being premised, select two tuning-forks the sounds of which differ by any consonant interval excepting the octave; place the broad sides of their branches, while in vibration, close to one ear, in such a manner that they shall nearly touch at the acoustic axis; the resulting grave harmonic will then be strongly audible, combined with the two other sounds; place afterwards one fork to each ear, and the consonance will be heard much richer in volume, but no audible indications whatever of the third sound will be perceived.[22]

Wheatstone's reference to the perceptual fusion of harmonically related tones were directly related to the principles examined by Wells. However, both their observations were ignored and remained uncited by contemporaraneous and subsequent German researchers of the following decades.
Venturi's experiments were repeated and confirmed by Lord Rayleigh (1842–1919), almost seventy-five years later.[23][24][25][26][27][28][29][30]

Other investigators of the late eighteenth and early nineteenth centuries, who were contemporaries of Lord Rayleigh, also investigated the significance of binaural hearing. These included Louis Trenchard More (1870-1944), a professor of physics, and Harry Shipley Fry (1878-1949), a lecturer in chemistry, both at the University of Cincinnati; H. A. Wilson and Charles Samuel Myers, both professors of science at King's College London; and Alfred M. Mayer (1836 - 1897), an American physicist, each of whom conducted experimental investigations with intent to discover the means by which human subjects ascertain the location, origin, and direction of sound, believing this to be in some way dependent on dichotic hearing, that is listening to sound through both ears.[31][32][33][34]

Understanding of how the difference in sound signal between two ears contributes to auditory processing in such a way as to enable the location and direction of sound to be determined was considerably advanced after the invention of the differential stethophone by Somerville Scott Alison in 1859, who coined the term 'binaural'. Alison based his stethophone on the stethoscope, a previous invention of René Théophile Hyacinthe Laennec (1781–1826).[35]

Unlike the stethoscope, which had only a single sound-source piece placed upon the chest, Alison's stethophone had two separate ones, allowing the user to hear and compare sounds derived from two discreet locations. This allowed a physician to identify the source of a sound through the process of binaural hearing. Subsequently, Alison referred to his invention as a 'binaural stethoscope', describing it as:

…an instrument consisting of two hearing-tubes, or trumpets, or stethoscopes, provided with collecting-cups and ear-knobs, one for each ear respectively. The two tubes are, for convenience, mechanically combined, but may be said to be acoustically separate, as care is taken that the sound, once admitted into one tube, is not communicated to the other.[36][37]

 

Neurophysiology

 

Cortical Oscillation and Electroencephalography (EEG)


The activity of neurons generate electric currents; and the synchronous action of neural ensembles in the cerebral cortex, comprising large numbers of neurons, produce macroscopic oscillations, which can be monitored and graphically documented by an electroencephalogram (EEG). The electroencephalographic representations of those oscillations are typically denoted by the term 'brainwaves' in common parlance.[38][39]

Neural oscillations are rhythmic or repetitive electrochemical activity in the brain and central nervous system. Such oscillations can be characterized by their frequency, amplitude and phase. Neural tissue can generate oscillatory activity driven by mechanisms within individual neurons, as well as by interactions between them. They may also adjust frequency to synchronize with the periodicity of an external acoustic or visual stimuli.[40]

The technique of recording neural electrical activity within the brain from electrochemical readings taken from the scalp originated with the experiments of Richard Caton in 1875, whose findings were developed into electroencephalography (EEG) by Hans Berger in the late 1920s.

 

Frequency bands of cortical neural ensembles


The fluctuating frequency of oscillations generated by the synchronous activity of cortical neurons, measurable with an electroencephalogram (EEG), via electrodes attached to the scalp, are conveniently categorized into general bands, in order of decreasing frequency, measured in Hertz (HZ) as follows:[41][42]

In addition, three further wave forms are often delineated in electroencephalographic studies:

It was Berger who first described the frequency bands Delta, Theta, Alpha, and Beta.

 

Neurophysiological origin of binaural beat perception


Binaural-beat perception originates in the inferior colliculus of the midbrain and the superior olivary complex of the brainstem, where auditory signals from each ear are integrated and precipitate electrical impulses along neural pathways through the reticular formation up the midbrain to the thalamus, auditory cortex, and other cortical regions.[44][45][46][47]

 

Neural oscillations and mental state


Following the technique of measuring such brainwaves by Berger, there has remained a ubiquitous consensus that electroencephalogram (EEG) readings depict brainwave wave form patterns that alter over time, and correlate with the aspects of the subject's mental and emotional state, mental status, and degree of consciousness and vigilance.[48][49][50] It is therefore now established and accepted that discreet electroencephalogram (EEG) measurements, including frequency and amplitude of neural oscillations, correlate with different perceptual, motor and cognitive states.[51][52][53][54][55][56][57][58][59][60][61]

Furthermore, brainwaves alter in response to changes in environmental stimuli, including sound and music; and while the degree and nature of alteration is partially dependent on individual perception, such that the same stimulus may precipitate differing changes in neural oscillations and correlating electroencephalogram (EEG) readings in different subjects, the frequency of cortical neural oscillations, as measured by the EEG, has also been shown to synchronize with or entrain to that of an external acoustic or photic stimulus, with accompanying alterations in cognitive and emotional state. This process is called neuronal entrainment or brainwave entrainment.

 

Entrainment

 

Meaning and Origin of the Term 'Entrainment'


Entrainment is a term originally derived from complex systems theory, and denotes the way that two or more independent, autonomous oscillators with differing rhythms or frequencies, when situated in a context and at a proximity where they can interact for long enough, influence each other mutually, to a degree dependent on coupling force, such that they adjust until both oscillate with the same frequency. Examples include the mechanical entrainment or cyclic synchronization of two electric clothes dryers placed in close proximity, and the biological entrainment evident in the synchronized illumination of fireflies.[62]

Entrainment is a concept first identified by the Dutch physicist Christiaan Huygens in 1665 who discovered the phenomenon during an experiment with pendulum clocks: He set them each in motion and found that when he returned the next day, the sway of their pendulums had all synchronized.[63]

Such entrainment occurs because small amounts of energy are transferred between the two systems when they are out of phase in such a way as to produce negative feedback. As they assume a more stable phase relationship, the amount of energy gradually reduces to zero, with system of greater frequency slowing down, and the other speeding up.[64]

Subsequently, the term 'entrainment' has been used to describe a shared tendency of many physical and biological systems to synchronize their periodicity and rhythm through interaction. This tendency has been identified as specifically pertinent to the study of sound and music generally, and acoustic rhythms specifically. The most ubiquitous and familiar examples of neuromotor entrainment to acoustic stimuli is observable in spontaneous foot or finger tapping to the rhythmic beat of a song.

 

Exogenous entrainment


Exogenous rhythmic entrainment, which occurs outside the body, has been identified and documented for a variety of human activities, which include the way people adjust the rhythm of their speech patterns to those of the subject with whom they communicate, and the rhythmic unison of an audience clapping.[65]

Even among groups of strangers, the rate of breathing, locomotive and subtle expressive motor movements, and rhythmic speech patterns have been observed to synchronize and entrain, in response to an auditory stimuli, such as a piece of music with a consistent rhythm.[66][67][68][69][70][71][72] Furthermore, motor synchronization to repetitive tactile stimuli occurs in animals, including cats and monkeys as well as humans, with accompanying shifts in electroencephalogram (EEG) readings.[73][74][75][76][77]

 

Endogenous entrainment


Examples of endogenous entrainment, which occurs within the body, include the synchronizing of human circadian sleep-wake cycles to the 24-hour cycle of light and dark.[78] and the synchronization of a heartbeat to a cardiac pacemaker.[79]

 

Brainwave entrainment

Main article: Brainwave entrainment

Brainwaves, or neural oscillations, share the fundamental constituents with acoustic and optical wave forms, including frequency, amplitude, and periodicity. Consequently, Huygens' discovery precipitated inquiry into whether or not the synchronous electrical activity of cortical neural ensembles might not only alter in response to external acoustic or optical stimuli but also entrain or synchronize their frequency to that of a specific stimulus.[80][81][82][83]

Brainwave entrainment is a colloquialism for such 'neural entrainment', which is a term used to denote the way in which the aggregate frequency of oscillations produced by the synchronous electrical activity in ensembles of cortical neurons can adjust to synchronize with the periodicity of an external stimuli, such as a sustained acoustic frequency perceived as pitch, a regularly repeating pattern of intermittent sounds, perceived as rhythm, or a regularly rhythmically intermittent flashing light.

 

The frequency following response and auditory driving


The hypothesized entrainment of neural oscillations to the frequency of an acoustic stimulus occurs by way of the Frequency following response (FFR), also referred to as Frequency Following Potential (FFP). The use of sound with intent to influence brainwave cortical brainwave frequency is called auditory driving.[84][85]
Auditory driving refers to the hypothesized ability for repetitive rhythmic auditory stimuli to 'drive' neural electric activity to entrain with it. By the principles of such hypotheses, it is proposed that, for example, a subject who hears drum rhythms at 8 beats per second, will be influenced such that an electroencephalogram (EEG) reading will show an increase brainwave activity at 8 Hz range, in the upper theta, lower alpha band.

 

Binaural beats and neural entrainment


One of the problems inherent in any scientific investigation conducted in order to ascertain whether brainwaves can entrain to the frequency of an acoustic stimulus is that human subjects rarely hear frequencies below 20 Hz, which is exactly the range of Delta, Theta, Alpha, and low to mid Beta brainwaves.[86][87] Among the methods by which some investigations have sought to overcome this problem is to measure electroencephalogram (EEG) readings of a subject while he or she listens to binaural beats. Subsequent to such investigations, there is significant evidence to show that such listening precipitates auditory driving by which ensembles of cortical neurons entrain their frequencies to that of the binaural beat, with associated changes in self-reported subjective experience of emotional and cognitive state.[88][89][90][91][92][93][94][95][96][97][98][99][100][101][102][103]

 

Binaural beats and music


Many of the aforementioned reports are based on the use of auditory stimuli that combines binaural beats with other sounds, including music and verbal guidance. This consequently precludes the attribution of any influence on or positive outcome for the listener specifically to the perception of the binaural beats.[104] Very few studies have sought to isolate the effect of binaural beats on listeners. However, initial findings in one experiment suggest that listening to binaural beats may exert an influence on both Low Frequency and High

Frequency components of heart rate variability, and may increase subjective feelings of relaxation.[105]
Notwithstanding this problem, a review of research findings suggest that listening to music and sound can modulate autonomic arousal through entrainment of neural oscillations. Furthermore, music generally, and rhythmic patterns, such as those produced by percussive performance including drumming specifically, have been shown to influence arousal ergotropically and trophotropically, increasing and decreasing arousal respectively.[106] Such auditory stimulation has been demonstrated to improve immune function, facilitate relaxation, improve mood, and contribute to the alleviation of stress.[107][108][109][110][111][112][113][114]

Meanwhile, the therapeutic benefits of listening to sound and music, whether or not the outcome can be attributed to neural entrainment, is a well-established principle upon which the practice of receptive music therapy is founded. The term 'receptive music therapy' denotes a process by which patients or participants listen to music with specific intent to therapeutically benefit; and is a term used by therapists to distinguish it from 'active music therapy' by which patients or participants engage in producing vocal or instrumental music.[115]

Receptive music therapy is an effective adjunctive intervention suitable for treating a range of physical and mental conditions.[116]

Meanwhile, the evident changes in neural oscillations precipitated by listening to music, which are demonstrable through electroencephalogram (EEG) measurements,[117][118][119][120][121][122] have contributed to the development of neurologic music therapy, which uses music and song as an active and receptive intervention, to contribute to the treatment and management of disorders characterized by impairment to parts of the brain and central nervous system, including stroke, traumatic brain injury, Parkinson's disease, Huntington's disease, cerebral palsy, Alzheimer's disease, and autism.[123][124][125]

 

Non ordinary states of consciousness


Historically, music generally, and percussive performance specifically was and remains integral to ritual ceremony and spiritual practice among early and indigenous peoples and their descendants, where it is often used to induce the non ordinary state of consciousness (NOSC) believed by participants to be a requisite for communication with spiritual energies and entities.[126][127]

While there is no scientific evidence for existence of such energy or entities, and thereby nor the human capacity to communicate with them, the findings of some contemporary research suggests that listening to rhythmic sounds, especially percussion, can induce the subjective experience of a non ordinary states of consciousness (NOSC), with correlating electroencephalogram (EEG) profiles comparable to those associated with some forms of meditation, while also increasing the susceptibility to hypnosis.[128][129][130][131] Specifically, some investigations show that the electroencephalogram (EEG) readings attained while a subject is meditating are comparable to those taken while he or she is listening to binaural beats, characterized by increased activity in the Alpha and Theta bands.[132][133][134][135][136]

 

See also

 

References




  • McConnell, P. A., Froeliger, B., Garland, E. L., Ives, J. C., & Sforzo, G. A., Auditory driving of the autonomic nervous system: Listening to theta-frequency binaural beats post-exercise increases parasympathetic activation and sympathetic withdrawal. Frontiers in Psychology, Vol. 5, p2014.
  • Draganova R., Ross B., Wollbrink A., Pantev C. (2008). Cortical steady-state responses to central and peripheral auditory beats. Cerebral Cortex Vol. 18, 2008, pp1193–1200.
  • Stumpf, C., Binaurale Tonmischung, Mehrheitsschwelle und Mitteltonbildung, Zeitschrift für Psychologie Vol. 75, 1916, pp330-350.
  • Wade, N. J. and Ono, H., From dichoptic to dichotic: historical contrasts between binocular vision and binaural hearing, Perception Vol. 34, 2005, pp645-668.
  • Beyer, R. T., Sounds of Our Times: Two Hundred Years of Acoustics. Mellville, NY: American Institute of Physics, 1998.
  • Alison, S. S., On the differential stethophone, and some new phenomena observed by it, Proceedings of the Royal Society of London 9,1859, pp196-209.
  • Wells, W. C., An Essay upon Single Vision with two Eyes: together with Experiments and Observations on several other Subjects in Optics. London: Cadell, 1792.
  • Wade, N. J., Destined for Distinguished Oblivion: The Scientific Vision of William Charles Wells (1757-1817). New York, NY: Kluwer-Plenum, 2003.
  • Venturi, J. B., Considérations sur la connaissance de l’étendue que nous donne le sens de l’ouïe,”Magasin Encyclopédique, ou Journal des Sciences, des Lettres et des Arts 3, 1796, pp29-37.
  • Venturi, J. B., Betrachtungen über die Erkenntniss des Raums durch den Sinn des Gohörs,” Magazin für den neuesten Zustand der Naturkunde 2, 1800, pp1-16.
  • Venturi, J. B., Riflessioni sulla conoscenza dello spazio, che noi possiamo ricavar dall’udito, in Indagine Fisica sui Colori by G. Venturi (Tipografica, Modena), 1801, pp. 133-149.
  • Venturi, J. B., Betrachtungen über die Erkenntniss der Entfernung, die wir durch das Werkzeug des Gehörs erhalten,” Archiv für die Physiologie 5, 1802, pp383-392.
  • Venturi, J. B., Riflessioni sulla conoscenza dello spazio, che noi possiamo ricavar dall’udito, in Indagine Fisica sui Colori by G. Venturi (Tipografica, Modena), 1801, pp. 133-149.
  • Venturi, J. B., Betrachtungen über die Erkenntniss der Entfernung, die wir durch das Werkzeug des Gehörs erhalten,” Archiv für die Physiologie 5, 1802, pp383-392.
  • Chladni, E. F. F., Entdeckungen über die Theorie des Klanges. Leipzig : Weidmanns Erben und Reich, 1787.

  • Chladni, E. F. F., Die Akustik. Leipzig: Breitkopf und Härtel, 1802.
  • Chladni, E. F. F., Traité d’Acoustique (Paris: Courcier, 1809.
  • Seebeck, A., Beiträge zur Physiologie des Gehör- und Gesichtssinnes, Annalen der Physik und Chemie Vol. 68, 1846, pp449-465.
  • Wade, N. J., Destined for Distinguished Oblivion: The Scientific Vision of William Charles Wells (1757-1817). New York, NY: Kluwer-Plenum, 2003.
  • Wade, N. J., A Natural History of Vision, Cambridge, MA: MIT Press, 1998.
  • Wade, N. J. and Ono, H., From dichoptic to dichotic: historical contrasts between binocular vision and binaural hearing, Perception Vol. 34, 2005, pp645-668.
  • Wheatstone, C., Experiments on audition, Quarterly Journal of Science, Literature and Art, Vol. 24, 1827, pp67-72.
  • Lord Rayleigh, Our perception of the direction of a source of sound, Nature Vol. 7, 1876, pp32-33.
  • Lord Rayleigh, On Our Perception of the Direotion of a Source of Sound. Proceedings of the Musical Association, Vol. 2, No. 1, 1875, pp75-84.
  • Lord Rayleigh, Acoustical observations. III. The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science, Vol. 9, No. 56, 1880, pp278-283.
  • Lord Rayleigh, On our perception of sound direction, Philosophical Magazine, Series 6, Vol. 13, No. 74, 1907, pp214-232.
  • Lord Rayleigh, Acoustical notes, Philosophical Magazine, Series 6, Vol. 13, No. 75, 1907, pp316-333.
  • Lord Rayleigh, Acoustical observations. Philosophical Magazine Series 5, Vol. 3, No. 20, 1877, pp.456-464.
  • Lord Rayleigh, Acoustical observations, The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science, Vol. 9, No. 56, 1880, pp278-283.
  • Lord Rayleigh, Acoustical observations, Philosophical Magazine, Series 5, Vol. 13, No. 82, 1882, pp340-347.
  • Beyer, R. T., Sounds of Our Times: Two Hundred Years of Acoustics. Mellville, NY: American Institute of Physics, 1998.
  • More, L. T. and Fry, H. S., On the appreciation of difference of phase of sound-waves, Philosophical Magazine, Series 6, Vol. 13, No. 76, 1907, pp452-459.
  • Wilson, H. A. and Myers, C. S., The influence of binaural phase differences on the localisation of sounds, British Journal of Psychology, Vol. 2, No. 4, 1908, pp363–385.
  • Mayer, A. M., Researches in acoustics, Philosophical Magazine, Series 4, Vol. 49, No. 326, 1875, pp352-365.
  • Laennec, R. T. H., Traité de l'Auscultation Médiate. Paris: Chaudé, 1819.
  • Alison, S. S., The physical examination of the chest in pulmonary consumption and its intercurrent diseases. British and Foreign Medico-Chirurgical Review 28, 1861, pp145-154.
  • Alison, S. S., On the differential stethophone, and some new phenomena observed by it, Proceedings of the Royal Society of London 9,1859, pp196-209.
  • da Silva, F. L., Neural mechanisms underlying brain waves: from neural membranes to networks. Electroencephalography and Clinical Neurophysiology, Vol. 79, No. 2, 1991, pp81-93.
  • Cooper, R., Winter, A., Crow, H., and Walter, W. G., Comparison of subcortical, cortical, and scalp activity using chronically indwelling electrodes in man. Electroencephalography and Clinical Neurophysiology, Vol. 18, 1965, pp217–230.
  • Niedermeyer E. and da Silva F.L., Electroencephalography: Basic Principles, Clinical Applications, and Related Fields. Lippincot Williams & Wilkins, 2004.
  • da Silva, F. H., and van Leeuwan, W., The cortical alpha rhythm in and the depth and surface profile of phase. In Brazier, M. A. B. and Petsche, H., (Eds.), Architectonics of the Cerebral Cortex. New York, NY: Raven Press, 1978.
  • da Silva, F. H., Neural mechanism underlying brain waves: From neural membranes to networks. Electroencephalography and Clinical Neurophysiology, Vol. 79, 1991, pp81–93.
  • Deuschl, G., and Eisen, A., Recommendations for the practice of clinical neurophysiology. Guidelines of the International Federation of Clinical Neurophysiology. Electroencephalography and Clinical Neurophysiology Supplement, 1999.
  • Smith J. C., Marsh J. T. and Brown W. S. Far-field recorded frequency-following responses: evidence for the locus of brainstem sources. Electroencephalogr. Clin. Neurophysiol. Vol., 1975, pp465–472.
  • Oster, G., Auditory beats in the brain. Scientific American, Vol. 229, No. 4, 1973, pp94-102.
  • Swann R., Bosanko S., Cohen R., Midgley R., Seed K. M.,The Brain - A User’s Manual. New York, NY: G. P. Putnam and Sons, 1982.
  • Draganova R., Ross B., Wollbrink A., Pantev C., Cortical steady-state responses to central and peripheral auditory beats. Cerebral Cortex Vol. 18, 2008, pp1193-1200.
  • Trzepacz, P. T., and Baker, R. W., The psychiatric mental status examination. Oxford, UK: Oxford University Press, 1993.
  • Engel, A. K., and Singer, W., Temporal binding and the neural correlates of sensory awareness. Trends in cognitive sciences, Vol. 5, No. 1, 2001, pp16-25.
  • Varela, F., Lachaux, J. P., Rodriguez, E., and Martinerie, J.,The brainweb: phase synchronization and large-scale integration. Nature Reviews Neuroscience, Vol. 2, No. 4, 2001, pp229-239.
  • Anokhin, A. P., Lutzenberger, W., and Birbaumer, N., Spatiotemporal organization of brain dynamics and intelligence: An EEG study in adolescents. The International Journal of Psychophysiology, Vol. 33, 1999, pp259–273.
  • Başar, E., Başar-Eroglu, C., Karakas, S., and Schürmann, M., Brain oscillations in perception and memory. International Journal of Psychophysiology, Vol. 35, 2000, pp95–124.
  • Burgess, A. P., and Gruzelier, J. H., Short duration synchronization of human theta rhythm during recognition memory. NeuroReport, 8, 1997, pp1039-1042.
  • Eckhorn, R., Bauer, R., Jordan, W., Brosch, M., Kruse, W., Munk, M., and Reitboeck, H. J., Coherent oscillations: A mechanism of feature linking in the visual cortex? Multiple electrode and correlation analyses in the cat. Biological Cybernetics, Vol. 60, 1988, pp121–130.
  • Engel, A. K., Konig, P., Kreiter, A. K., & Singer, W., Interhemispheric synchronization of oscillatory neuronal responses in cat visual cortex. Nature, Vol. 252, 1991, pp1177-1179.
  • Klimesch, W., EEG alpha and theta oscillations reflect cognitive and memory performance: A review and analysis. Brain Research Reviews, Vol. 29, 1999, pp169-195.
  • Klimesch, W., Schimke, H., & Schwaiger, J., Episodic and semantic memory: An analysis in the EEG theta and alpha band. Electroencephalography and Clinical Neurophysiology, Vol. 91, 1994, pp428-441.
  • Miltner, W. H. R., Braun, C., Arnold, M., Witte, M., and Taub, E., Coherence of gamma-band EEG activity as a basis for associative learning. Nature, Vol. 397, 1999, pp434-436.
  • Rodriguez, E., George, N., Lachaux, J., Martinerie, J., Renault, B., and Varela, F., Perceptions shadow: Long-distance synchronization of human brain activity. Nature, Vol. 397, 1999, pp430–433.
  • Tallon-Baudry, C., Bertrand, O., and Fischer, C., Oscillatory synchrony between human extrastriate areas during visual short-term memory maintenance. Journal of Neuroscience, Vol. 21, No. 15, 2001, RC177.
  • Tallon, C., Bertrand, O., Bouchet, P., and Pernier, J. (1995). Gamma-range activity evoked by coherent visual stimuli in humans. European Journal of Neuroscience, Vol. 7, 1995, pp1285-1291.
  • Néda, Z., Ravasz, E., Brechet, Y., Vicsek, T., & Barabsi, A. L., Self-organizing process: The sound of many hands clapping. Nature, Vol. 403, 2000, pp849–850.
  • Pantaleone, J., Synchronization of Metronomes. American Journal of Physics, Vol. 70, 2002 pp992–1000.
  • Bennett, M., Schatz, M. F., Rockwood, H., and Wiesenfeld, K., Huygens's clocks. Proceedings: Mathematics, Physical and Engineering Sciences, 2002, pp563-579.
  • Néda, Z., Ravasz, E., Brechet, Y., Vicsek, T., & Barabsi, A. L., Self-organizing process: The sound of many hands clapping. Nature, Vol. 403, 2000, pp849–850.
  • Haas, F., Distenfeld, S., & Axen, K., Effects of perceived musical rhythm on respiratory pattern. Journal of Applied Physiology, Vol. 61, No. 3, 1986, pp1185–1191.
  • Safranek, M., Koshland, G., and Raymond, G., Effect of auditory rhythm on muscle activity. Physical Therapy, Vol. 62, 1982, pp161–168.
  • Thaut, M.H., Schleiffers, S., and Davis, W.B., Changes in EMG patterns under the influence of auditory rhythm. In Spintge, R. and Droh, R. (Eds.), Music Medicine St. Louis, MO: MMB Music, 1992.
  • Thaut, M. H., McIntosh, G. C., Prassas, S. G., and Rice, R. R., Effect of rhythmic cuing on temporal stride parameters and EMG patterns in hemiparetic stroke patients. Journal of Neurologic Rehabilitation, Vol. 7, 1993, pp9–16.
  • Thaut, M., McIntosh, G., Prassas, S., and Rice, R., Effect of rhythmic cuing on temporal stride parameters and EMG patterns in normal gait. Journal of Neurologic Rehabilitation, Vol. 6, 1992, pp185–190.
  • McIntosh, G.C., Thaut, M.H., and Rice, R.R., 1996. Rhythmic auditory stimulation as entrainment and therapy technique in gait of stroke and Parkinson’s disease patients. In Pratt, R. and. Spintge, R., (Eds.), Music Medicine. St. Louis, MO: MMB Music, 1996.
  • Condon, W. S., Multiple response to sound in dysfunctional children. Journal of Autism and Childhood Schizophrenia, Vol. 5, No. 1, 1975, p43.
  • Pompeiano, O., and Swett, J. E., EEG and behavioral manifestations of sleep induced by cutaneous nerve stimulation in normal cats. Archives Italiennes de Biologie, Vol. 100, 1962, pp311–342.
  • Walter, D. O., and Adey, W. R., Linear and nonlinear mechanisms of brainwave generation. Annals of the New York Academy of Sciences, Vol. 128, 1966, pp772–780.
  • Namerow, N. S., Sclabassi, R. J., and Enns, N. F., Somatosensory responses to stimulus trains: Normative data. Electroencephalography and Clinical Neurophysiology, Vol. 37, 1974, pp11–21.
  • Gavalas, R. J., Walter, D. O., Hamer, J., and Adey, W. R., Effects of low-level, low-frequency electric fields on EEG and behavior in Macaca uemestriua. Brain Research, Vol. 18, 1970, pp491–501.
  • Buzsáki, G., Rhythms of the Brain. New York, NY: Oxford University Press, 2006.
  • Clayton M., Sager R., and Will U., In time with the music: the concept of entrainment and its significance for ethnomusicology. In European Meetings in Ethnomusicology Vol. 11, 2005, pp3-142.
  • Cvetkovic D., Powers R., and Cosic I., Preliminary evaluation of electroencephalographic entrainment using thalamocortical modelling. Expert Systems, Vol. 26, 2009, pp320-338.
  • Will, U., and Berg, E., Brainwave synchronization and entrainment to periodic stimuli. Neuroscience Letters, Vol. 424, 2007, pp55–60.
  • Cade, G. M. and Coxhead, F., The awakened mind, biofeedback and the development of higher states of awareness. New York, NY: Delacorte Press, 1979.
  • Neher, A., Auditory driving observed with scalp electrodes in normal subjects. Electroencephalography and Clinical Neurophysiology, Vol. 13, 1961, pp449–451.
  • Zakharova, N. N., and Avdeev, V. M., Functional changes in the central nervous system during music perception. Zhurnal vysshei nervnoi deiatelnosti imeni IP Pavlova Vol. 32, No. 5, 1981, pp915-924.
  • Burkard, R., Don, M., and Eggermont, J. J., Auditory evoked potentials: Basic principles and clinical application. Philadelphia, PA: Lippincott Williams & Wilkins, 2007.
  • Worden, F.G.; Marsh, J.T., Frequency-following (microphonic-like) neural responses evoked by sound. Electroencephalography and Clinical Neurophysiology Vol. 25, No. 1, 1968, pp42–52.
  • Rosen, S. and Howell, P., Signals and Systems for Speech and Hearing. Bingley, UK: Emerald, 2001.
  • Rossing, T., (2007). Springer Handbook of Acoustics. Berlin, Springer: 2007.
  • Wahbeh, H., Calabrese, C., and Zwickey, H., Binaural beat technology in humans: a pilot study to assess psychologic and physiologic effects. The Journal of Alternative and Complementary Medicine, Vol. 13, No. 1, 2007, pp25-32.
  • Becher, A. K., Höhne, M., Axmacher, N., Chaieb, L., Elger, C. E., and Fell, J., Intracranial electroencephalography power and phase synchronization changes during monaural and binaural beat stimulation. European Journal of Neuroscience, Vol. 41, No. 2, 2015, pp254-263.
  • Solcà, M., Mottaz, A., and Guggisberg, A. G, Binaural beats increase interhemispheric alpha-band coherence between auditory cortices. Hearing research, 2015.
  • Guruprasath, G., and Gnanavel, S., Effect of continuous and short burst binaural beats on EEG signals. In Innovations in Information, Embedded and Communication Systems (ICIIECS), 2015 International Conference, 2015, IEEE.
  • Jirakittayakorn, N., and Wongsawat, Y., The brain responses to different frequencies of binaural beat sounds on QEEG at cortical level. In Engineering in Medicine and Biology Society (EMBC), 2015. 37th Annual International Conference of the IEEE, 2015.
  • Becher, A. K., Höhne, M., Axmacher, N., Chaieb, L., Elger, C. E., and Fell, J. (2015). Intracranial electroencephalography power and phase synchronization changes during monaural and binaural beat stimulation. European Journal of Neuroscience, Vol. 41, No. 2, 2015, pp254-263.
  • Mihajloski, T. (2015). Characterization of Auditory Evoked Potentials From Transient Binaural beats Generated by Frequency Modulating Sound Stimuli. Doctoral Thesis, University of Miami, 2015.
  • Becher, A. K., Höhne, M., Axmacher, N., Chaieb, L., Elger, C. E., and Fell, J., Intracranial electroencephalography power and phase synchronization changes during monaural and binaural beat stimulation. European Journal of Neuroscience, Vol. 41, No. 2, 2015, pp254-263.
  • Vernon, D., Peryer, G., Louch, J., and Shaw, M.,Tracking EEG changes in response to alpha and beta binaural beats. International Journal of Psychophysiology, Vol. 93, No. 1, 2014, pp134-139.
  • Gao, X., Cao, H., Ming, D., Qi, H., Wang, X., Wang, X., ... and Zhou, P., Analysis of EEG activity in response to binaural beats with different frequencies. International Journal of Psychophysiology, Vol. 94, No. 3, 2014, pp399-406.
  • Forster, J., Bader, L., Heßler, S., Roesler, O., and Suendermann, D. A., First Step Towards Binaural Beat Classification Using Multiple EEG Devices. In Proceedings of the International Conference on Applied Informatics for Health and Life Sciences, Kusadasi, Turkey, October 2014.
  • On, F. R., Jailani, R., Norhazman, H., and Zaini, N. M., Binaural beat effect on brainwaves based on EEG. In Signal Processing and its Applications (CSPA), 2013 IEEE 9th International Colloquium, 2013, IEEE.
  • Kasprzak, C. (2011). Influence of binaural beats on EEG signal. Acta physica polonica, Vol. 119, No. 6A, 2011, pp986-990.
  • Pratt, H., Starr, A., Michalewski, H. J., Dimitrijevic, A., Bleich, N., and Mittelman, N., Cortical evoked potentials to an auditory illusion: binaural beats. Clinical neurophysiology, Vol. 120, No. 8, 2009, pp1514-1524.
  • Karino, S., Yumoto, M., Itoh, K., Uno, A., Yamakawa, K., Sekimoto, S., and Kaga, K. (2006). Neuromagnetic responses to binaural beat in human cerebral cortex. Journal of neurophysiology, Vol. 96, No. 4, 2006, pp1927-1938.
  • Cvetkovic, D., Cosic, I., and Djuwari, D.,The induced rhythmic oscillations of neural activity in the human brain. In Proceedings of IASTED (Biomedical Engineering), 2004.
  • McConnell, P. A., Froeliger, B., Garland, E. L., Ives, J. C., & Sforzo, G. A., Auditory driving of the autonomic nervous system: Listening to theta-frequency binaural beats post-exercise increases parasympathetic activation and sympathetic withdrawal. Frontiers in Psychology, Vol. 5, 2014.
  • McConnell, P. A., Froeliger, B., Garland, E. L., Ives, J. C., & Sforzo, G. A., Auditory driving of the autonomic nervous system: Listening to theta-frequency binaural beats post-exercise increases parasympathetic activation and sympathetic withdrawal. Frontiers in Psychology, Vol. 5, 2014.
  • Trost W. and Vuilleumier P., Rhythmic entrainment as a mechanism for emotion induction by music: a neurophysiological perspective. In The Emotional Power of Music: Multidisciplinary Perspectives on Musical Arousal, Expression, and Social Control, Cochrane T., Fantini B., and Scherer K. R., (Eds.), Oxford, UK: Oxford University Press; 2013, pp213–225.
  • Szabó, C., The effects of monotonous drumming on subjective experiences. Music Therapy Today, Vol. 1, 2004, 2004, pp. 1-9.
  • Bittman, B. B., Berk, L. S., Felten, D. L., Westengard, J., Simonton, O. C., Pappas, J., and Ninehouser, M., Composite effects of group drumming music therapy on modulation of neuroendocrine-immune parameters in normal subjects. Alternative Therapeutic Health Medicine, Vol. 1, 2001, pp38–47.
  • Wachiuli, M., Koyama, M., Utsuyama, M., Bittman, B. B., Kitagawa, M., and Hirokawa, K., Recreational music-making modulates natural killer cell activity, cytokines, and mood states in corporate employees. Medical Science Monitor, Vol. 13, No. 2, 2007, CR57–70.

  • Bittman, B., Bruhn, K. T., Stevens, C., & Westengard, J., and Umbach, P. O., Recreational music-making: A cost-effective group interdisciplinary strategy for reducing burnout and improving mood states in long-term care workers. Advanced Mind Body Medicine, Vol. 19, Nos. 3-4, 2003, p16.
  • Bittman, B. B., Snyder, C., Bruhn, K. T., Liebfreid, F., Stevens, C. K., Westengard, J., and Umbach, P. O., Recreational music-making: An integrative group intervention for reducing burnout and improving mood states in first year associate degree nursing students: Insights and economic impact. International Journal of Nursing Education Scholarship, Vol. 1, Article 12, 2004.
  • Walton, K., and Levitsky, D., A neuroendocrine mechanism for the reduction of drug use and addictions by transcendental meditation. In O’Connell, D. and Alexander, C. (Eds.), Self-recovery: Treating addictions using transcendental meditation and Maharishi Ayur-Veda. New York, NY: Haworth, 1994.
  • Szabó, C., The effects of monotonous drumming on subjective experiences. Music Therapy Today, Vol. 1, 2004, pp. 1–9.
  • Winkelman, M., Complementary therapy for addiction: Drumming out drugs. The American Journal of Public Health, Vol. 93, 2003, pp647–651.
  • Bruscia, K., Defining music therapy. Barcelona: Gilsum, NH, 1998.
  • Grocke, D., and Wigram, T. (2007). Receptive methods in music therapy: Techniques and clinical applications for music therapy clinicians, educators, and students. London, England: Jessica Kingsley, 2007.
  • Wagner, M. J., Brainwaves and biofeedback. A brief history - Implications for music research. Journal of Music Therapy, Vol. 12, No. 2, 1975, pp46-58.
  • Fikejz, F., Influence of music on human electroencephalogram. In Applied Electronics (AE), International Conference, 2011.
  • Ogata, S., Human EEG responses to classical music and simulated white noise: effects of a musical loudness component on consciousness. Perceptual and Motor Skills Vol. 80, No. 3, 1995, pp779-790.
  • Lin, Y. P., Yang, Y. H., and Jung, T. P., Fusion of electroencephalographic dynamics and musical contents for estimating emotional responses in music listening. Frontiers in Neuroscience, Vol. 8, 2014.
  • Nakamura, S., Sadato, N., Oohashi, T., Nishina, E., Fuwamoto, Y., and Yonekura, Y., Analysis of music–brain interaction with simultaneous measurement of regional cerebral blood flow and electroencephalogram beta rhythm in human subjects. Neuroscience letters, Vol. 275, No. 3, 1999, pp222-226.
  • Karthick, N. G., Thajudin, A. V. I., and Joseph, P. K., Music and the EEG: a study using nonlinear methods. In Biomedical and Pharmaceutical Engineering, 2006. Biomedical and Pharmaceutical Engineering, International Conference, Singapore, 2006.
  • Thaut, M. H., Peterson, D. A., & McIntosh, G. C. (2005). Temporal entrainment of cognitive functions. Annals of the New York Academy of Sciences, 1060(1), 243-254
  • Thaut, M.,Training manual for neurologic music therapy. Colorado State University: Center for Biomedical Research in Music, 1999.
  • Thaut, M. H., Neurologic music therapy in cognitive rehabilitation. Music Perception, Vol. 27, No. 4, 2010, pp281-285.
  • Winkelman, M. (1997). Altered states of consciousness and religious behavior. In Glazier, S., (Ed.), Anthropology of Religion: A Handbook of Method and Theory. Westport, CT: Greenwood Press, 1997.
  • Rouget, G., Music and Trance: A Theory of the Relations Between Music and Possession. Chicalgo, IL: University of Chicago Press, 1985.
  • Maurer, R. L., Sr., Kumar, V. K., Woodside, L., and Pekala, R. J., Phenomenological experience in response to monotonous drumming and hypnotizability. American Journal of Clinical Hypnosis, Vol. 40, No. 2, 1997, pp130–145.
  •  Mandell, A., Toward a psychobiology of transcendence: God in the brain. In Davidson, D. and Davidson, R., (Eds.), The Psychobiology of Consciousness New York, NY: Plenum Press, 1980.



  • Winkelman, M., Shamanism: The Neural Ecology of Consciousness and Healing. Westport, CT: Bergin and Garvey, 2000.
  • Stevens, L., Haga, Z., Queen, B., Brady, B., Adams, D., Gilbert, J., and McManus, P., Binaural beat induced theta EEG activity and hypnotic susceptibility: contradictory results and technical considerations. American Journal of Clinical Hypnosis, Vol. 45, No. 4, 2003, pp295-309.
  • Yamsa-ard, T., and Wongsawat, Y., The observation of theta wave modulation on brain training by 5 Hz-binaural beat stimulation in seven days. In Engineering in Medicine and Biology Society (EMBC), 37th Annual International Conference of the IEEE, 2015.
  • Gifari, M. W., Said, S. M., Lam, J., JALIL, N., and Supriyanto, E. Binaural Beat Entrainment Effect on Prefrontal and Parietal Brain EEG in Theta Frequency. Proceedings of the 11th International Conference on Cellular and Molecular Biology, Biophysics and Bioengineering, 2015.
  • Pfaff, H. U., Psychophysiological reactivity to auditory Binaural Beats stimulation in the alpha and theta EEG brain-wave frequency bands: A randomized, double–blind and placebo–controlled study in human healthy young adult subjects. Masters Thesis. Universidad Autonoma Madrid, 2014.
  • Yamsa-ard, T., and Wongsawat, Y., The relationship between EEG and binaural beat stimulation in meditation. In Proceedings of the Biomedical Engineering International Conference (BMEiCON), 2014, IEEE.
  • Puzi, N. M., Jailani, R., Norhazman, H., and Zaini, N. M. (2013, March). Alpha and Beta brainwave characteristics to binaural beat treatment. In Signal Processing and its Applications (CSPA), 9th International Colloquium, 2013, IEEE.

  •  

    Further reading

    • Thaut, M. H., Rhythm, Music, and the Brain: Scientific Foundations and Clinical Applications (Studies on New Music Research). New York, NY: Routledge, 2005.
    • Berger, J. and Turow, G. (Eds.), Music, Science, and the Rhythmic Brain : Cultural and Clinical Implications. New York, NY: Routledge, 2011.

     

    External links

    Saturday, December 15, 2012

    Water Sphere in Zero Gravity



    In his off-duty time, NASA Astronaut Don Pettit experiments with the physics of water in the weightless environment aboard the International Space Station. Published as a collaboration between NASA and the American Physical Society See: Science Off the Sphere



    See Also:

    Friday, December 14, 2012

    It's Final Endgame for GRAIL's Twin Spacecraft


    The mountain where the two spacecraft will make contact is located near a crater named Goldschmidt. Both spacecraft have been flying in formation around the moon since Jan. 1, 2012. They were named by elementary school students in Bozeman, Mont., who won a contest. The first probe to reach the moon, Ebb, also will be the first to go down, at 2:28:40 p.m. PST. Flow will follow Ebb about 20 seconds later. See: NASA Probes Prepare for Mission-Ending Moon Impact



    GRAIL's Final Resting Spot
    These maps of Earth's moon highlight the region where the twin spacecraft of NASA's Gravity Recovery and Interior Laboratory (GRAIL) mission will impact on Dec. 17, marking the end of its successful endeavor to map the moon's gravity. The two washing-machine-sized spacecraft, named Ebb and Flow, will impact at an unnamed mountain near the moon's North Pole. These maps are from NASA's Lunar Reconnaissance Orbiter.
    Credit: NASA/GSFC



    See Also:


    Thursday, December 13, 2012

    See 21-23 January 2013 CERN


    The primary goal of this 3‐day workshop is to educate the LHC community about the scientific utility of likelihoods. We shall do so by describing and discussing several real‐world examples of the use of likelihoods, including a one‐day in‐depth examination of likelihoods in the Higgs boson studies by ATLAS and CMS.
    The workshop will start with two pedagogical lectures that introduce likelihood concepts and terminology. These lectures are followed, in the afternoon of Day 1, by a moderated discussion that focuses on the concepts and issues raised in the lectures. Day 1 ends with several presentations that illustrate the use of likelihoods in Higgs and Beyond the Standard Model (BSM) research. The goal here is to get feedback from researchers who have used Higgs and BSM results in their work.See: Likelihood for the LHC Searches

    LHC data publications of the last 12 months

    Just keeping tally of archived research material at Cern.

    ALICE

    • Pseudorapidity density of charged particles p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV, http://arxiv.org/abs/1210.3615, Phys. Rev. Lett..
    • Transverse Momentum Distribution and Nuclear Modification Factor of Charged Particles in p-Pb Collisions at $\sqrt{s_{NN}}$ = 5.02 TeV, http://arxiv.org/abs/1210.4520, Phys. Rev. Lett..
    • Coherent J/$\Psi$ photoproduction in ultra-peripheral Pb-Pb collisions at $\sqrt{s_{NN}}$ =2.76 TeV, http://arxiv.org/abs/1209.3715, Phys. Lett. B.
    • Measurement of inelastic, single- and double-diffraction cross sections in proton-proton collisions at the LHC with ALICE, http://arxiv.org/abs/1208.4968, Eur. Phys. J. C.
    • Measurement of electrons from beauty hadron decays in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1208.1902.
    • Centrality Dependence of Charged Particle Production at Large Transverse Momentum in Pb--Pb Collisions at $\sqrt{s_{\rm{NN}}} = 2.76$ TeV, http://arxiv.org/abs/1208.2711, Phys. Lett. B.
    • Pion, Kaon, and Proton Production in Central Pb--Pb Collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1208.1974, Phys. Rev. Lett..
    • D$_s^+$ meson production at central rapidity in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1208.1948.
    • Production of $K*(892)^0$ and $\phi$(1020) in pp collisions at $\sqrt{s}$ =7 TeV, http://arxiv.org/abs/1208.5717, Eur. Phys. J. C, 72: 2183, 2012.
    • Net-Charge Fluctuations in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV, http://arxiv.org/abs/1207.6068.
    • Charge separation relative to the reaction plane in Pb-Pb collisions at $\sqrt{s_{NN}}$= 2.76 TeV, http://arxiv.org/abs/1207.0900.
    • K$^{0}_{s}$-K$^{0}_{s}$ correlations in pp collisions at $\sqrt{s}$=7 TeV from the LHC ALICE experiment, http://arxiv.org/abs/1206.2056.
    • Production of muons from heavy flavour decays at forward rapidity in pp and Pb-Pb collisions at $\sqrt {s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1205.6443, Phys. Rev. Lett..
    • Anisotropic flow of charged hadrons, pions and (anti-)protons measured at high transverse momentum in Pb-Pb collisions at $\sqrt{s_{NN}}$=2.76 TeV, http://arxiv.org/abs/1205.5761.
    • Transverse sphericity of primary charged particles in minimum bias proton-proton collisions at $\sqrt{s}$=0.9, 2.76 and 7 TeV, http://arxiv.org/abs/1205.3963.
    • Measurement of charm production at central rapidity in proton-proton collisions at $\sqrt{s}$ = 2.76 TeV, http://arxiv.org/abs/1205.4007, J. High Energy Phys., 07: 191, 2012.
    • Measurement of prompt and non-prompt J/$\psi$ production cross sections at mid-rapidity in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1205.5880.
    • Measurement of electrons from semileptonic heavy-flavour hadron decays in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1205.5423.
    • Multi-strange baryon production in pp collisions at $\sqrt{s}$ = 7 TeV with ALICE, http://arxiv.org/abs/1204.0282, Phys. Lett. B, 712: 309-318, 2012.
    • Suppression of high transverse momentum D mesons in central Pb--Pb collisions at $\sqrt{s_{NN}}=2.76$ TeV, http://arxiv.org/abs/1203.2160.
    • Measurement of the Cross Section for Electromagnetic Dissociation with Neutron Emission in Pb-Pb Collisions at √sNN = 2.76 TeV, http://arxiv.org/abs/1203.2436.
    • Inclusive J/$\psi$ production in pp collisions at $\sqrt{s}$ = 2.76 TeV, http://arxiv.org/abs/1203.3641, Phys. Lett. B, 718: 295-306, 2012.
    • J/$\psi$ Production as a Function of Charged Particle Multiplicity in pp Collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.2816, Phys. Lett. B.
    • Heavy flavour decay muon production at forward rapidity in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1201.3791, Phys. Lett. B, 708: 265-275, 2012.
    • J/$\psi$ production at low transverse momentum in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1202.1383, Phys. Rev. Lett..
    • Measurement of Event Background Fluctuations for Charged Particle Jet Reconstruction in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1201.2423, J. High Energy Phys., 03: 053, 2012.
    • Neutral pion and $\eta$ meson production in proton-proton collisions at $\sqrt{s}$=0.9 TeV and $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1205.5724.

    ATLAS

    • Search for a heavy narrow resonance decaying to $e\mu, e\tau$, or $\mu\tau$ with the ATLAS detector in $\sqrt{s}$ = 7 TeV pp collisions at the LHC, http://arxiv.org/abs/1212.1272, Phys. Lett. B.
    • Measurement of Upsilon production in 7 TeV pp collisions at ATLAS, http://arxiv.org/abs/1211.7255, Phys. Rev. D.
    • Measurement of the $t\bar{t}$ production cross section in the tau+jets channel using the ATLAS detector, http://arxiv.org/abs/1211.7205, Eur. Phys. J. C.
    • Search for new phenomena in events with three charged leptons at a center-of-mass energy of 7 TeV with the ATLAS detector, http://arxiv.org/abs/1211.6312, Phys. Rev. D.
    • Measurement of ZZ production in pp collisions at $\sqrt{s}$=7 TeV and limits on anomalous ZZZ and ZZ$\gamma$ couplings with the ATLAS detector, http://arxiv.org/abs/1211.6096, J. High Energy Phys..
    • Search for resonances decaying into top-quark pairs using fully hadronic decays in pp collisions with ATLAS at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1211.2202, J. High Energy Phys..
    • Measurement of isolated-photon pair production in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1211.1913, J. High Energy Phys..
    • Searches for heavy long-lived sleptons and R-Hadrons with the ATLAS detector in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1211.1597, Phys. Lett. B.
    • Search for contact interactions and large extra dimensions in dilepton events from pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1211.1150, Phys. Rev. D.
    • Search for supersymmetry in events with photons, bottom quarks, and missing transverse momentum in proton-proton collisions at a centre-of-mass energy of 7 TeV with the ATLAS detector, http://arxiv.org/abs/1211.1167, Phys. Lett. B.
    • Search for Extra Dimensions in diphoton events using proton-proton collisions recorded at $\sqrt{s}$ = 7 TeV with the ATLAS detector at the LHC, http://arxiv.org/abs/1210.8389, Phys. Lett. B.
    • Search for long-lived, heavy particles in final states with a muon and multi-track displaced vertex in proton-proton collisions at $\sqrt{s}$=7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.7451, Phys. Lett. B.
    • A search for high-mass resonances decaying to tau+tau- in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.6604, Phys. Lett. B.
    • Measurement of Z boson Production in Pb+Pb Collisions at $\sqrt{s_{NN}}$=2.76 TeV with the ATLAS Detector, http://arxiv.org/abs/1210.6486, Phys. Rev. Lett..
    • Jet energy resolution in proton-proton collisions at $\sqrt{s}$ = 7 TeV recorded in 2010 with the ATLAS detector, http://arxiv.org/abs/1210.6210, Eur. Phys. J. C.
    • Measurement of angular correlations in Drell-Yan lepton pairs to probe $Z/\gamma*$ boson transverse momentum at $\sqrt{s}$=7 TeV with the ATLAS detector, http://arxiv.org/abs/1211.6899, Phys. Lett., B.
    • Search for the neutral Higgs bosons of the Minimal Supersymmetric Standard Model in pp collisions at $\sqrt{s}$=7 TeV with the ATLAS detector, http://arxiv.org/abs/1211.6956, J. High Energy Phys..
    • Search for pair production of heavy top-like quarks decaying to a high-$p_T$ W boson and a b quark in the lepton plus jets final state at $\sqrt{s}$=7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.5468, Phys. Lett. B.
    • Search for doubly-charged Higgs bosons in like-sign dilepton final states at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.5070, Eur. Phys. J. C.
    • Search for pair-produced massive coloured scalars in four-jet final states with the ATLAS detector in proton-proton collisions at sqrt(s) = 7 TeV, http://arxiv.org/abs/1210.4826, Eur. Phys. J. C.
    • Search for pair production of massive particles decaying into three quarks with the ATLAS detector in $\sqrt{s}$ = 7 TeV pp collisions at the LHC, http://arxiv.org/abs/1210.4813, J. High Energy Phys..
    • Search for anomalous production of prompt like-sign lepton pairs at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.4538, J. High Energy Phys..
    • Search for dark matter candidates and large extra dimensions in events with a jet and missing transverse momentum with the ATLAS detector, http://arxiv.org/abs/1210.4491, J. High Energy Phys..
    • Search for R-parity-violating supersymmetry in events with four or more leptons in $\sqrt{s}$ = 7 TeV pp collisions with the ATLAS detector, http://arxiv.org/abs/1210.4457, J. High Energy Phys..
    • Measurement of $W^+W^-$ production in pp collisions at $\sqrt{s}$=7 TeV with the ATLAS detector and limits on anomalous WWZ and WW$_{\gamma}$ couplings, http://arxiv.org/abs/1210.2979, Phys. Rev. D.
    • Search for direct chargino production in anomaly-mediated supersymmetry breaking models based on a disappearing-track signature in pp collisions at $\sqrt{s}$=7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.2852, J. High Energy Phys..
    • ATLAS search for new phenomena in dijet mass and angular distributions using pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1210.1718, J. High Energy Phys..
    • Search for Supersymmetry in Events with Large Missing Transverse Momentum, Jets, and at Least One Tau Lepton in 7 TeV Proton-Proton Collision Data with the ATLAS Detector, http://arxiv.org/abs/1210.1314, Eur. Phys. J. C, 72: 2215, 2012.
    • Search for resonant top quark plus jet production in $t\bar{t}$+jets events with the ATLAS detector in pp collisions at $\sqrt{s}$=7  TeV, http://arxiv.org/abs/1209.6593, Phys. Rev. D, 86: 091103(R), 2012.
    • Search for dark matter candidates and large extra dimensions in events with a photon and missing transverse momentum in pp collision data at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1209.4625, Phys. Rev. Lett..
    • ATLAS search for a heavy gauge boson decaying to a charged lepton and a neutrino in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1209.4446, Eur. Phys. J. C.
    • Search for a heavy top-quark partner in final states with two leptons with the ATLAS detector at the LHC, http://arxiv.org/abs/1209.4186, J. High Energy Phys., 11: 094, 2012.
    • Search for high-mass resonances decaying to dilepton final states in pp collisions at a center-of-mass energy of 7 TeV with the ATLAS detector, http://arxiv.org/abs/1209.2535, J. High Energy Phys..
    • Search for light top squark pair production in final states with leptons and b-jets with the ATLAS detector in $\sqrt{s}$ = 7 TeV proton-proton collisions, http://arxiv.org/abs/1209.2102, Phys. Lett. B.
    • Search for diphoton events with large missing transverse momentum in 7 TeV proton-proton collision data with the ATLAS detector, http://arxiv.org/abs/1209.0753, Phys. Lett. B, 718: 411-430, 2012.
    • Measurements of the pseudorapidity dependence of the total transverse energy in proton-proton collisions at $\sqrt{s}$ = 7 TeV with ATLAS, http://arxiv.org/abs/1208.6256, J. High Energy Phys..
    • Measurement of the flavour composition of dijet events in pp collisions at $\sqrt{s}$=7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.0441, Eur. Phys. J. C.
    • Further search for supersymmetry at $\sqrt{s}$ = 7 TeV in final states with jets, missing transverse momentum and isolated leptons with the ATLAS detector, http://arxiv.org/abs/1208.4688, Phys. Rev. D, 86: 092002, 2012.
    • Search for light scalar top-quark pair production in final states with two leptons with the ATLAS detector in $\sqrt{s}$ = 7 TeV proton-proton collisions, http://arxiv.org/abs/1208.4305, Eur. Phys. J. C, 72: 2237, 2012.
    • Search for direct production of charginos and neutralinos in events with three leptons and missing transverse momentum in $\sqrt{s}$ = 7 TeV pp collisions with the ATLAS detector, http://arxiv.org/abs/1208.3144, Phys. Lett. B.
    • Search for direct slepton and gaugino production in final states with two leptons and missing transverse momentum with the ATLAS detector in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1208.2884, Phys. Lett. B.
    • Search for new phenomena in the $WW \to l\nu l' \nu'$ final state in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1208.2880, Phys. Lett. B.
    • Search for direct top squark pair production in final states with one isolated lepton, jets, and missing transverse momentum in $\sqrt{s}$ = 7 TeV pp collisions using 4.7 fb$^{-1}$ of ATLAS data, http://arxiv.org/abs/1208.2590, Phys. Rev. Lett., 109: 211803, 2012.
    • Search for displaced muonic lepton jets from light Higgs boson decay in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1210.0435, Phys. Lett. B.
    • Measurement of the jet radius and transverse momentum dependence of inclusive jet suppression in lead-lead collisions at $\sqrt{s_{NN}}$ = 2.76 TeV with the ATLAS detector, http://arxiv.org/abs/1208.1967, Phys. Lett. B.
    • Search for a supersymmetric partner to the top quark in final states with jets and missing transverse momentum at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1208.1447, Phys. Rev. Lett., 109: 211802, 2012.
    • Measurement of W$^{\pm}$Z production in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1208.1390, Eur. Phys. J. C, 72: 2173, 2012.
    • Search for squarks and gluinos with the ATLAS detector in final states with jets and missing transverse momentum using 4.7 fb$^{-1}$ of $\sqrt{s}$ = 7 TeV proton-proton collision data, http://arxiv.org/abs/1208.0949, Phys. Rev. D.
    • Time-dependent angular analysis of the decay $B_s^0 \to J/\psi \phi$ and extraction of $\Delta \Gamma_s$ and the CP-violating weak phase $\phi_s$ by ATLAS, http://arxiv.org/abs/1208.0572, J. High Energy Phys..
    • Underlying event characteristics and their dependence on jet size of charged-particle jet events in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1208.0563, Phys. Rev. D, 86: 072004, 2012.
    • Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC, http://arxiv.org/abs/1207.7214, Phys. Lett. B, 716: 1-29, 2012.
    • Measurement of charged-particle event shape variables in $\sqrt{s}$ = 7 TeV proton-proton interactions with the ATLAS detector, http://arxiv.org/abs/1207.6915, Phys. Rev. D.
    • Search for magnetic monopoles in $\sqrt{s}$ = 7 TeV pp collisions with the ATLAS detector, http://arxiv.org/abs/1207.6411, Phys. Rev. Lett..
    • Measurements of top quark pair relative differential cross-sections with ATLAS in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.5644, Eur. Phys. J. C.
    • Search for top and bottom squarks from gluino pair production in final states with missing transverse energy and at least three b-jets with the ATLAS detector, http://arxiv.org/abs/1207.4686, Eur. Phys. J. C, 72: 2174, 2012.
    • A search for $t\bar{t}$ resonances in lepton+jets events with highly boosted top quarks collected in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1207.2409, J. High Energy Phys., 09: 041, 2012.
    • Measurement of the $\Lambda_b^0$ lifetime and mass in the ATLAS experiment, http://arxiv.org/abs/1207.2284, Phys. Rev. D.
    • Combined search for the Standard Model Higgs boson in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1207.0319, Phys. Rev. D, 86: 032003, 2012.
    • Search for the Standard Model Higgs boson produced in association with a vector boson and decaying to a b-quark pair with the ATLAS detector, http://arxiv.org/abs/1207.0210, Phys. Lett. B, 718: 369-390, 2012.
    • Search for the Standard Model Higgs boson in the $H \to \tau^+ \tau^-$ decay mode in $\sqrt{s}$ = 7 TeV pp collisions with ATLAS, http://arxiv.org/abs/1206.5971, J. High Energy Phys., 09: 070, 2012.
    • Search for the Higgs boson in the $H \to WW \to l\nu jj$ decay channel at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1206.6074, Phys. Lett. B, 718: 391-410, 2012.
    • ATLAS measurements of the properties of jets for boosted particle searches, http://arxiv.org/abs/1206.5369, Phys. Rev. D, 86: 072006, 2012.
    • Measurement of the b-hadron production cross section using decays to $D^{*+}\mu^- X$ final states in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1206.3122, Nucl. Phys. B, 864: 341-381, 2012.
    • Search for a Standard Model Higgs boson in the mass range 200-600 GeV in the $H \to ZZ \to l^+l^-q\bar{q}$ decay channel with the ATLAS detector, http://arxiv.org/abs/1206.2443, Phys. Lett. B, 717: 70–88, 2012.
    • Measurement of event shapes at large momentum transfer with the ATLAS detector in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.2135, Eur. Phys. J. C, 72: 2211, 2012.
    • Hunt for new phenomena using large jet multiplicities and missing transverse momentum with ATLAS in 4.7 fb$^{-1}$ of $\sqrt{s}$ = 7 TeV proton-proton collisions, http://arxiv.org/abs/1206.1760, J. High Energy Phys., 07: 167, 2012.
    • Search for the Standard Model Higgs boson in the $H \to WW^{(*)} \to l\nu l\nu$ decay mode with 4.7 fb$^{-1}$ of ATLAS data at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.0756, Phys. Lett. B, 716: 62-81, 2012.
    • A search for flavour changing neutral currents in top-quark decays in pp collision data collected with the ATLAS detector at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.0257, J. High Energy Phys., 09: 139, 2012.
    • Search for a Standard Model Higgs boson in the $H \to ZZ \to l^+l^-\nu\bar{\nu}$ decay channel using 4.7 fb$^{-1}$ of $\sqrt{s}$ = 7 TeV data with the ATLAS detector, http://arxiv.org/abs/1205.6744, Phys. Lett. B, 717: 29-48, 2012.
    • Evidence for the associated production of a W boson and a top quark in ATLAS at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1205.5764, Phys. Lett. B, 716: 142-159, 2012.
    • A search for $t\bar{t}$ resonances with the ATLAS detector in 2.05 fb$^{-1}$ of proton-proton collisions at $\sqrt(s)$ = 7 TeV, http://arxiv.org/abs/1205.5371, Eur. Phys. J. C, 72: 2083, 2012.
    • Search for tb resonances in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1205.1016, Phys. Rev. Lett., 109: 081801, 2012.
    • Measurement of the t-channel single top-quark production cross section in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1205.3130, Phys. Lett. B, 717: 330-350, 2012.
    • Measurement of $W\gamma$ and $Z\gamma$ production cross sections in pp collisions at $\sqrt{s}$ = 7 TeV and limits on anomalous triple gauge couplings with the ATLAS detector, http://arxiv.org/abs/1205.2531, Phys. Lett. B, 717: 49-69, 2012.
    • Measurement of the W boson polarization in top quark decays with the ATLAS detector, http://arxiv.org/abs/1205.2484, J. High Energy Phys., 06: 088, 2012.
    • Measurement of the top quark pair cross section with ATLAS in pp collisions at $\sqrt{s}$ = 7 TeV using final states with an electron or a muon and a hadronically decaying $\tau$ lepton, http://arxiv.org/abs/1205.2067, Phys. Lett. B, 717: 89-108, 2012.
    • Search for lepton flavour violation in the $e\mu$ continuum with the ATLAS detector in $\sqrt{s}$ = 7 TeV pp collisions at the LHC, http://arxiv.org/abs/1205.0725, Eur. Phys. J. C, 72: 2040, 2012.
    • Search for scalar top quark pair production in natural gauge mediated supersymmetry models with the ATLAS detector in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.6736, Phys. Lett. B, 715: 44-60, 2012.
    • Measurement of $\tau$ polarization in $W \to \tau\nu$ decays with the ATLAS detector in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.6720, Eur. Phys. J. C, 72: 2062, 2012.
    • Search for supersymmetry in events with three leptons and missing transverse momentum in $\sqrt{s}$ = 7 TeV pp collisions with the ATLAS detector, http://arxiv.org/abs/1204.5638, Phys. Rev. Lett., 108: 261804, 2012.
    • Searches for TeV-scale Gravity Signatures in Final States with Leptons and Jets with the ATLAS Detector at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.4646, Phys. Lett. B, 716: 122-141, 2012.
    • Search for supersymmetry with jets, missing transverse momentum and at least one hadronically decaying tau lepton in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1204.3852, Phys. Lett. B, 714: 197-214, 2012.
    • Search for charged Higgs bosons decaying via $H^{\pm} \to \tau \nu$ in $t\bar{t}$ events using pp collision data at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1204.2760, J. High Energy Phys., 06: 039, 2012.
    • Search for resonant WZ production in the $WZ \to l\nu l'l'$ channel in $\sqrt{s}$ = 7 TeV pp collisions with the ATLAS detector, http://arxiv.org/abs/1204.1648, Phys. Rev. D, 85: 112012, 2012.
    • Search for Pair Production of a New b′ Quark that Decays into a Z Boson and a Bottom Quark with the ATLAS Detector, http://arxiv.org/abs/1204.1265, Phys. Rev. Lett., 109: 071801, 2012.
    • Search for the decay $B_s^0 \to \mu^+ \mu^-$ with the ATLAS detector, http://arxiv.org/abs/1204.0735, Phys. Lett. B, 713: 387, 2012.
    • Search for a fermiophobic Higgs boson in the diphoton decay channel with the ATLAS detector, http://arxiv.org/abs/1205.0701, Eur. Phys. J. C, 72: 2157, 2012.
    • Search for events with large missing transverse momentum, jets, and at least two tau leptons in 7 TeV proton-proton collision data with the ATLAS detector, http://arxiv.org/abs/1203.6580, Phys. Lett. B, 714: 180-196, 2012.
    • Measurement of the WW cross section in $\sqrt{s}$ = 7 TeV pp collisions with the ATLAS detector and limits on anomalous gauge couplings, http://arxiv.org/abs/1203.6232, Phys. Lett. B, 712: 289-308, 2012.
    • Search for supersymmetry in pp collisions at $\sqrt{s}$ = 7 TeV in final states with missing transverse momentum and b-jets with the ATLAS detector, http://arxiv.org/abs/1203.6193, Phys. Rev. D, 85: 112006, 2012.
    • Search for gluinos in events with two same-sign leptons, jets and missing transverse momentum with the ATLAS detector in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1203.5763, Phys. Rev. Lett., 108: 241802, 2012.
    • Measurement of the top quark mass with the template method in the top antitop $\to$ lepton + jets channel using ATLAS data, http://arxiv.org/abs/1203.5755, Eur. Phys. J. C, 72: 2046, 2012.
    • Search for heavy neutrinos and right-handed W bosons in events with two leptons and jets in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1203.5420, Eur. Phys. J. C, 72: 2056, 2012.
    • Measurement of $t\overline{t}$ production with a veto on additional central jet activity in pp collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector, http://arxiv.org/abs/1203.5015, Eur. Phys. J. C, 72: 2043, 2012.
    • Jet mass and substructure of inclusive jets in $\sqrt{s}$ = 7 TeV pp collisions with the ATLAS experiment, http://arxiv.org/abs/1203.4606, J. High Energy Phys., 05: 128, 2012.
    • Measurement of the charge asymmetry in top quark pair production in $pp$ collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector, http://arxiv.org/abs/1203.4211, Eur. Phys. J. C, 72: 2039, 2012.
    • Observation of spin correlation in $t\overline{t}$ events from $pp$ collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector, http://arxiv.org/abs/1203.4081, Phys. Rev. Lett., 108: 212001, 2012.
    • Determination of the strange quark density of the proton from ATLAS measurements of the $W \to l\nu$ and $Z \to ll$ cross sections, http://arxiv.org/abs/1203.4051, Phys. Rev. Lett., 109: 012001, 2012.
    • Search for second generation scalar leptoquarks in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1203.3172, Eur. Phys. J. C, 72: 2151, 2012.
    • Measurement of the production cross section of an isolated photon associated with jets in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1203.3161, Phys. Rev. D, 85: 092014, 2012.
    • Forward-backward correlations and charged-particle azimuthal distributions in $pp$ interactions using the ATLAS detector, http://arxiv.org/abs/1203.3100, J. High Energy Phys., 07: 019, 2012.
    • Measurement of the azimuthal anisotropy for charged particle production in $\sqrt{s_{NN}}$ = 2.76 TeV lead-lead collisions with the ATLAS detector, http://arxiv.org/abs/1203.3087, Phys. Rev. C, 86: 014907, 2012.
    • Measurement of the polarisation of W bosons produced with large transverse momentum in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS experiment, http://arxiv.org/abs/1203.2165, Eur. Phys. J. C, 72: 2001, 2012.
    • Search for a light Higgs boson decaying to long-lived weakly-interacting particles in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1203.1303, Phys. Rev. Lett., 108: 251801, 2012.
    • Single hadron response measurement and calorimeter jet energy scale uncertainty with the ATLAS detector at the LHC, http://arxiv.org/abs/1203.1302, Eur. Phys. J. C.
    • Search for new particles decaying to ZZ using final states with leptons and jets with the ATLAS detector in $\sqrt{s}$ = 7 Tev proton-proton collisions, http://arxiv.org/abs/1203.0718, Phys. Lett. B, 712: 331-350, 2012.
    • Search for FCNC single top-quark production at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1203.0529, Phys. Lett. B, 712: 351-369, 2012.
    • Measurement of the azimuthal ordering of charged hadrons with the ATLAS detector, http://arxiv.org/abs/1203.0419, Phys. Rev. D, 86: 052005, 2012.
    • Search for Down-Type Fourth Generation Quarks with the ATLAS Detector in Events with One Lepton and Hadronically Decaying W Bosons, http://arxiv.org/abs/1202.6540, Phys. Rev. Lett., 109: 032001, 2012.
    • Search for same-sign top-quark production and fourth-generation down-type quarks in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1202.5520, J. High Energy Phys., 04: 069, 2012.
    • Measurement of the cross section for top-quark pair production in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector using final states with two high-pt leptons, http://arxiv.org/abs/1202.4892, J. High Energy Phys., 05: 059, 2012.
    • Search for anomaly-mediated supersymmetry breaking with the ATLAS detector based on a disappearing-track signature in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.4847, Eur. Phys. J. C, 72: 1993, 2012.
    • Search for pair-produced heavy quarks decaying to Wq in the two-lepton channel at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1202.3389, Phys. Rev. D, 86: 012007, 2012.
    • Search for Pair Production of a Heavy Up-Type Quark Decaying to a W Boson and a b Quark in the lepton+jets Channel with the ATLAS Detector, http://arxiv.org/abs/1202.3076, Phys. Rev. Lett., 108: 261802, 2012.
    • Search for the Standard Model Higgs boson in the decay channel $H \to ZZ^{(*)} \to 4l$ with 4.8 fb$^{-1}$ of pp collisions at $\sqrt{s}$=7 TeV with ATLAS, http://arxiv.org/abs/1202.1415, Phys. Lett. B, 710: 383-402, 2012.
    • Combined search for the Standard Model Higgs boson using up to 4.9 fb$^{-1}$ of pp collision data at $\sqrt{s}$ = 7 TeV with the ATLAS detector at the LHC, http://arxiv.org/abs/1202.1408, Phys. Lett. B, 710: 49-66, 2012.
    • Search for the Standard Model Higgs boson in the diphoton decay channel with 4.9 fb$^{-1}$ of pp collisions at $\sqrt{s}$=7 TeV with ATLAS, http://arxiv.org/abs/1202.1414, Phys. Rev. Lett., 108: 111803, 2012.
    • Search for decays of stopped, long-lived particles from 7 TeV pp collisions with the ATLAS detector, http://arxiv.org/abs/1201.5595, Eur. Phys. J. C, 72: 1965, 2012.
    • Measurement of inclusive two-particle angular correlations in pp collisions with the ATLAS detector at the LHC, http://arxiv.org/abs/1203.3549, J. High Energy Phys., 05: 157, 2012.
    • Search for excited leptons in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1201.3293, Phys. Rev. D, 85: 072003, 2012.
    • Rapidity gap cross sections measured with the ATLAS detector in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1201.2808, Eur. Phys. J. C, 72: 1926, 2012.
    • Measurement of the top quark pair production cross-section with ATLAS in the single lepton channel, http://arxiv.org/abs/1201.1889, Phys. Lett. B, 711: 244-263, 2012.
    • Study of jets produced in association with a W boson in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1201.1276, Phys. Rev. D, 85: 092002, 2012.
    • Search for anomalous production of prompt like-sign muon pairs and constraints on physics beyond the Standard Model with the ATLAS detector, http://arxiv.org/abs/1201.1091, Phys. Rev. D, 85: 032004, 2012.
    • Jet energy measurement with the ATLAS detector in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1112.6426, Eur. Phys. J. C.
    • Measurement of inclusive jet and dijet production in pp collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector, http://arxiv.org/abs/1112.6297, Phys. Rev. D, 86: 014022, 2012.
    • Search for heavy vector-like quarks coupling to light quarks in proton-proton collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1112.5755, Phys. Lett. B, 712: 22-39, 2012.
    • Observation of a new $\chi_b$ state in radiative transitions to $\Upsilon$(1S) and $\Upsilon$(2S) at ATLAS, http://arxiv.org/abs/1112.5154, Phys. Rev. Lett., 108: 152001, 2012.
    • Search for first generation scalar leptoquarks in pp collisions at $\sqrt{s}$=7 TeV with the ATLAS detector, http://arxiv.org/abs/1112.4828, Phys. Lett. B, 711: 442-455 (Erratum), 2012.
    • Search for contact interactions in dilepton events from pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1112.4462, Phys. Lett. B, 712: 40-58, 2012.
    • Measurement of $D^{*\pm}$ meson production in jets from pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1112.4432, Phys. Rev. D, 85: 052005, 2012.
    • Search for scalar bottom pair production with the ATLAS detector in pp Collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1112.3832, Phys. Rev. Lett., 108: 181802, 2012.
    • Search for production of resonant states in the photon-jet mass distribution using pp collisions at $\sqrt{s}$ = 7 TeV collected by the ATLAS detector, http://arxiv.org/abs/1112.3580, Phys. Rev. Lett., 108: 211802, 2012.
    • Search for the Higgs boson in the $H \to WW^{(*)} \to l^{+}\nu l^{-}\bar\nu$ decay channel in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector, http://arxiv.org/abs/1112.2577, Phys. Rev. Lett., 108: 111802, 2012.
    • Search for Extra Dimensions using diphoton events in 7 TeV proton-proton collisions with the ATLAS detector, http://arxiv.org/abs/1112.2194, Phys. Lett. B, 710: 538-556, 2012.

    CMS

    • Search for heavy resonances in the W/Z-tagged dijet mass spectrum in pp collisions at 7 TeV, http://cdsweb.cern.ch/record/1498395.
    • Search for long-lived particles decaying to photons and missing energy in proton-proton collisions at sqrt(s) = 7 TeV, http://cdsweb.cern.ch/record/1498386.
    • Search for exotic resonances decaying into WZ/ZZ in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1211.5779, J. High Energy Phys..
    • Measurement of the ZZ production cross section and search for anomalous couplings in 2l2l' final states in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1211.4890, J. High Energy Phys..
    • Search for new physics in events with photons, jets, and missing transverse energy in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1211.4784, J. High Energy Phys..
    • Identification of b-quark jets with the CMS experiment, http://arxiv.org/abs/1211.4462, J. Instrum..
    • Search for Z' resonances decaying to $t\bar{t}$ in dilepton+jets final states in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1211.3338, Phys. Rev. D.
    • Search for supersymmetry in final states with a single lepton, b-quark jets, and missing transverse energy in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1211.3143, Phys. Rev. D.
    • Search in leptonic channels for heavy resonances decaying to long-lived neutral particles, http://arxiv.org/abs/1211.2472, J. High Energy Phys..
    • Measurement of differential top-quark pair production cross sections in pp colisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1211.2220.
    • Search for supersymmetry in final states with missing transverse energy and 0, 1, 2, or at least 3 b-quark jets in 7 TeV pp collisions using the variable alphaT, http://arxiv.org/abs/1210.8115.
    • Measurement of the sum of WW and WZ production with W+dijet events in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.7544, Eur. Phys. J. C.
    • Search for heavy quarks decaying into a top quark and a W or Z boson using lepton + jets events in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.7471, J. High Energy Phys..
    • Search for a non-standard-model Higgs boson decaying to a pair of new light bosons in four-muon final states, http://arxiv.org/abs/1210.7619, Phys. Lett. B.
    • Measurement of the inelastic proton-proton cross section at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.6718, Phys. Lett. B.
    • Search for pair production of third-generation leptoquarks and top squarks in pp collisions at sqrt(s) = 7 TeV, http://arxiv.org/abs/1210.5629, Phys. Rev. Lett..
    • Search for third-generation leptoquarks and scalar bottom quarks in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.5627, J. High Energy Phys..
    • Observation of long-range near-side angular correlations in proton-lead collisions at the LHC, http://arxiv.org/abs/1210.5482, Phys. Lett. B.
    • Observation of Z decays to four leptons with the CMS detector at the LHC, http://arxiv.org/abs/1210.3844, J. High Energy Phys..
    • Search for fractionally charged particles in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.2311, Phys. Rev. Lett..
    • Search for heavy neutrinos and W$_R$ bosons with right-handed couplings in a left-right symmetric model in pp collisions at 7 TeV, http://arxiv.org/abs/1210.2402, Phys. Rev. Lett..
    • Search for narrow resonances and quantum black holes in inclusive and b-tagged dijet mass spectra from pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.2387, J. High Energy Phys..
    • Search for excited leptons in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.2422, Phys. Lett. B.
    • Search for supersymmetry in events with photons and low missing transverse energy in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.2052, Phys. Lett. B.
    • Search for heavy lepton partners of neutrinos in proton-proton collisions in the context of the type III seesaw mechanism, http://arxiv.org/abs/1210.1797, Phys. Lett. B, 718: 348-368, 2012.
    • Measurement of the relative prompt production rate of $\chi_{c2}$ and $\chi_{c1}$ in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.0875, Eur. Phys. J. C.
    • Search for anomalous production of highly boosted Z bosons decaying to dimuons in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1210.0867, Phys. Lett. B.
    • Search for electroweak production of charginos and neutralinos using leptonic final states in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1209.6620, J. High Energy Phys..
    • Measurement of the single-top-quark t-channel cross section in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1209.4533, J. High Energy Phys..
    • Search for resonant $t\bar{t}$ production in lepton+jets events in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1209.4397, J. High Energy Phys..
    • Search for the standard model Higgs boson produced in association with W and Z bosons in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1209.3937, J. High Energy Phys., 11: 088, 2012.
    • Search for a narrow spin-2 resonance decaying to a pair of Z vector bosons in the semileptonic final state, http://arxiv.org/abs/1209.3807, Phys. Lett. B.
    • Evidence for associated production of a single top quark and W boson in pp collisions at 7 TeV, http://arxiv.org/abs/1209.3489, Phys. Rev. Lett..
    • Measurement of the Y(1S), Y(2S) and Y(3S) polarizations in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1209.2922, Phys. Rev. Lett..
    • Measurement of the top-quark mass in $t\bar{t}$ events with dilepton final states in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1209.2393, Eur. Phys. J. C, 72: 2202, 2012.
    • Measurement of the top-quark mass in $t\bar{t}$ events with lepton+jets final states in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1209.2319, J. High Energy Phys..
    • Observation of a diffractive contribution to dijet production in proton-proton collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1209.1805, Phys. Rev. D.
    • Search for exclusive or semi-exclusive $\gamma\gamma$ production and observation of exclusive and semi-exclusive $e^+e^−$ production in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1209.1666, J. High Energy Phys., 11: 080, 2012.
    • Combined search for the quarks of a sequential fourth generation, http://arxiv.org/abs/1209.1062, Phys. Rev. D.
    • Search for pair produced fourth-generation up-type quarks in pp collisions at $\sqrt{s}$=7 TeV with a lepton in the final state, http://arxiv.org/abs/1209.0471, Phys. Lett. B, 718: 307-328, 2012.
    • Search for supersymmetry in events with b-quark jets and missing transverse energy in pp collisions at 7 TeV, http://arxiv.org/abs/1208.4859, Phys. Rev. D, 86: 072010, 2012.
    • Study of the dijet mass spectrum in pp $\to$ W + jets events at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1208.3477, Phys. Rev. Lett..
    • Search for three-jet resonances in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1208.2931, Phys. Lett. B, 718: 329-347, 2012.
    • Observation of sequential Upsilon suppression in PbPb collisions, http://arxiv.org/abs/1208.2826, Phys. Rev. Lett..
    • Measurement of the $t\bar{t}$ production cross section in the dilepton channel in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1208.2671, J. High Energy Phys..
    • Measurement of the azimuthal anisotropy of neutral pions in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1208.2470, Phys. Rev. Lett..
    • Search for flavor changing neutral currents in top quark decays in pp collisions at 7 TeV, http://arxiv.org/abs/1208.0957, Phys. Lett. B.
    • Search for a W' boson decaying to a bottom quark and a top quark in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1208.0956, Phys. Lett. B.
    • Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC, http://arxiv.org/abs/1207.7235, Phys. Lett. B, 716: 30-61, 2012.
    • Search for pair production of first- and second-generation scalar leptoquarks in pp collisions at $\sqrt{s}$= 7 TeV, http://arxiv.org/abs/1207.5406, Phys. Rev. D, 86: 052013, 2012.
    • Search for heavy Majorana neutrinos in $\mu^{\pm}\mu^{\pm}$ + jets and $e^{\pm}e^{\pm}$ + jets events in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.6079, Phys. Lett. B, 717: 109-128, 2012.
    • Study of the inclusive production of charged pions, kaons, and protons in pp collisions at $\sqrt{s}$ = 0.9, 2.76, and 7 TeV, http://arxiv.org/abs/1207.4724, Eur. Phys. J. C, 72: 2164, 2012.
    • Forward-backward asymmetry of Drell-Yan lepton pairs in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.3973, Phys. Lett. B.
    • A search for a doubly-charged Higgs boson in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.2666, Eur. Phys. J. C, 72: 2189, 2012.
    • Measurement of the underlying event activity in pp collisions at $\sqrt{s}$ = 0.9 and 7 TeV with the novel jet-area/median approach, http://arxiv.org/abs/1207.2392, J. High Energy Phys., 08: 130, 2012.
    • Search for supersymmetry in hadronic final states using $M_{T2}$ in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.1798, J. High Energy Phys., 10: 018, 2012.
    • Search for new physics in the multijet and missing transverse momentum final state in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.1898, Phys. Rev. Lett., 109: 171803, 2012.
    • Search for a fermiophobic Higgs boson in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1207.1130, J. High Energy Phys., 09: 111, 2012.
    • Search for new physics with long-lived particles decaying to photons and missing energy in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.0627, J. High Energy Phys..
    • Inclusive and differential measurements of the $t\bar{t}$ charge asymmetry in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1207.0065, Phys. Lett. B, 717: 129-150, 2012.
    • Search for stopped long-lived particles produced in pp collisions at $\sqrt{s}$ =7 TeV, http://arxiv.org/abs/1207.0106, J. High Energy Phys., 08: 026, 2012.
    • Search for a light pseudoscalar Higgs boson in the dimuon decay channel in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.6326, Phys. Rev. Lett., 109: 121801, 2012.
    • Search for dark matter and large extra dimensions in monojet events in pp collisions at $\sqrt{s}$= 7 TeV, http://arxiv.org/abs/1206.5663, J. High Energy Phys..
    • Search for new physics in events with opposite-sign leptons, jets, and missing transverse energy in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.3949, Phys. Lett. B.
    • Search for charge-asymmetric production of W' bosons in top pair + jet events from pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.3921, Phys. Lett. B, 717: 351–370, 2012.
    • Measurement of the electron charge asymmetry in inclusive W production in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.2598, Phys. Rev. Lett., 109: 111806, 2012.
    • Search for high mass resonances decaying into $\tau$-lepton pairs in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.1725, Phys. Lett. B, 716: 82-102, 2012.
    • Search for narrow resonances in dilepton mass spectra in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1206.1849, Phys. Lett. B, 714: 158-179, 2012.
    • Search for a W′ or Techni-$\rho$ Decaying into WZ in pp Collisions at $\sqrt{s}$=7  TeV, http://arxiv.org/abs/1206.0433, Phys. Rev. Lett., 109: 141801, 2012.
    • Study of W boson production in PbPb and pp collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1205.6334, Phys. Lett. B, 715: 66-87, 2012.
    • Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy, http://arxiv.org/abs/1205.6615, Phys. Rev. Lett., 109: 071803, 2012.
    • Measurement of jet fragmentation into charged particles in pp and PbPb collisions at $\sqrt{s_{NN}}$= 2.76 TeV, http://arxiv.org/abs/1205.5872, J. High Energy Phys., 10: 087, 2012.
    • Search for a light charged Higgs boson in top quark decays in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1205.5736, J. High Energy Phys., 07: 143, 2012.
    • Search for new physics in events with same-sign dileptons and b-tagged jets in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1205.3933, J. High Energy Phys., 08: 110, 2012.
    • Measurement of the pseudorapidity and centrality dependence of the transverse energy density in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1205.2488, Phys. Rev. Lett., 109: 152303, 2012.
    • Measurement of the $\Lambda_b$ cross section and the $\overline{\Lambda}_b$ to $\Lambda_b$ ratio with J/$\psi\Lambda$ decays in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1205.0594, Phys. Lett. B, 714: 136-157, 2012.
    • Search for heavy long-lived charged particles in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1205.0272, Phys. Lett. B, 713: 408-433, 2012.
    • Studies of jet quenching using isolated-photon+jet correlations in PbPb and pp collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1205.0206, Phys. Lett. B.
    • Observation of a New $\Xi_{b}$ Baryon, http://arxiv.org/abs/1204.5955, Phys. Rev. Lett., 108: 252002, 2012.
    • Search for anomalous production of multilepton events in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1204.5341, J. High Energy Phys., 06: 169, 2012.
    • Search for leptonic decays of W' bosons in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1204.4764, J. High Energy Phys., 08: 023, 2012.
    • Search for physics beyond the standard model in events with a Z boson, jets, and missing transverse energy in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.3774, Phys. Lett. B, 716: 260-284, 2012.
    • Shape, transverse size, and charged hadron multiplicity of jets in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.3170, J. High Energy Phys., 06: 160, 2012.
    • Measurement of the mass difference between top and antitop quarks, http://arxiv.org/abs/1204.2807, J. High Energy Phys., 06: 109, 2012.
    • Search for anomalous $t \bar{t}$ production in the highly-boosted all-hadronic final state, http://arxiv.org/abs/1204.2488, J. High Energy Phys..
    • Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1204.1850, Phys. Rev. Lett., 109: 022301, 2012.
    • Measurement of the Z/$\gamma^*$+b-jet cross section in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.1643, J. High Energy Phys., 06: 126, 2012.
    • Measurement of the underlying event in the Drell-Yan process in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.1411, Eur. Phys. J. C, 72: 2080, 2012.
    • Measurement of the elliptic anisotropy of charged particles produced in PbPb collisions at nucleon-nucleon center-of-mass energy = 2.76 TeV, http://arxiv.org/abs/1204.1409, Phys. Rev. C.
    • Search for heavy bottom-like quarks in 4.9 inverse femtobarns of pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.1088, J. High Energy Phys., 05: 123, 2012.
    • Search for Dark Matter and Large Extra Dimensions in pp Collisions Yielding a Photon and Missing Transverse Energy, http://arxiv.org/abs/1204.0821, Phys. Rev. Lett., 108: 261803, 2012.
    • Ratios of dijet production cross sections as a function of the absolute difference in rapidity between jets in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.0696, Eur. Phys. J. C, 72: 2216, 2012.
    • Measurement of the top quark pair production cross section in pp collisions at $\sqrt{s}$ = 7 TeV in dilepton final states containing a $\tau$, http://arxiv.org/abs/1203.6810, Phys. Rev. D, 85: 112007, 2012.
    • Search for heavy, top-like quark pair production in the dilepton final state in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1203.5410, Phys. Lett. B, 716: 103-121, 2012.
    • Search for $B_s^0 \to \mu^+ \mu^-$ and $B^0 \to \mu^+ \mu^-$ decays, http://arxiv.org/abs/1203.3976, J. High Energy Phys., 04: 033, 2012.
    • Measurement of the cross section for production of b b-bar X, decaying to muons in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1203.3458, J. High Energy Phys., 06: 110, 2012.
    • Search for microscopic black holes in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.6396, J. High Energy Phys., 04: 061, 2012.
    • Search for quark compositeness in dijet angular distributions from pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.5535, J. High Energy Phys., 05: 055, 2012.
    • Jet momentum dependence of jet quenching in PbPb collisions at $\sqrt{s_{NN}}$=2.76 TeV, http://arxiv.org/abs/1202.5022, Phys. Lett. B, 712: 176-197, 2012.
    • Inclusive b-jet production in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1202.4617, J. High Energy Phys., 04: 084, 2012.
    • Search for the standard model Higgs boson decaying to bottom quarks in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1202.4195, Phys. Lett. B, 710: 284-306, 2012.
    • Search for neutral Higgs bosons decaying to tau pairs in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1202.4083, Phys. Lett. B, 713: 68-90, 2012.
    • Search for large extra dimensions in dimuon and dielectron events in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.3827, Phys. Lett. B, 711: 15-34, 2012.
    • Search for the standard model Higgs boson in the $H \to ZZ \to l^+l^- \tau^+ \tau^-$ decay channel in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1202.3617, J. High Energy Phys., 03: 081, 2012.
    • Search for the standard model Higgs boson in the $H \to ZZ \to 2l 2\nu$ channel in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.3478, J. High Energy Phys., 03: 040, 2012.
    • Study of high-$p_T$ charged particle suppression in PbPb compared to pp collisions at $\sqrt{s_{NN}}$=2.76 TeV, http://arxiv.org/abs/1202.2554, Eur. Phys. J. C, 72: 1945, 2012.
    • Search for the standard model Higgs boson in the decay channel $H \to ZZ \to 4 l$ in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.1997, Phys. Rev. Lett., 108: 111804, 2012.
    • Search for the standard model Higgs boson decaying into two photons in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1202.1487, Phys. Lett. B, 710: 403-425, 2012.
    • Search for the standard model Higgs boson decaying to $W^+ W^-$ in the fully leptonic final state in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.1489, Phys. Lett. B, 710: 91-113, 2012.
    • Search for a Higgs boson in the decay channel $H \to ZZ^{(*)} \to q\bar{q}l^-l^+$ in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.1416, J. High Energy Phys., 04: 036, 2012.
    • Combined results of searches for the standard model Higgs boson in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.1488, Phys. Lett. B, 710: 26-48, 2012.
    • Measurement of the inclusive production cross sections for forward jets and for dijet events with one forward and one central jet in pp collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1202.0704, J. High Energy Phys., 06: 036, 2012.
    • Suppression of non-prompt J$\psi$, prompt J$\psi$, and $\Upsilon$(1S) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1201.5069, J. High Energy Phys., 05: 063, 2012.
    • Centrality dependence of dihadron correlations and azimuthal anisotropy harmonics in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1201.3158, Eur. Phys. J. C, 72: 2012, 2012.
    • Measurement of isolated photon production in pp and PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV, http://arxiv.org/abs/1201.3093, Phys. Lett. B, 710: 256-277, 2012.
    • Measurement of the charge asymmetry in top-quark pair production in proton-proton collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1112.5100, Phys. Lett. B, 709: 28-49, 2012.

    LHCb

    • Measurement of $J/\psi$ production in $pp$ collisions at $\sqrt{s}=2.76$ TeV, http://arxiv.org/abs/1212.1045, J. High Energy Phys..
    • Implications of LHCb measurements and future prospects, http://arxiv.org/abs/1208.3355, Eur. Phys. J. C.
    • First observation of the $B_{s2}^\ast(5840)^0 \to B^{\ast+} K^-$ decay and properties of the orbitally excited $B^0_s$ mesons, http://arxiv.org/abs/1211.5994, Phys. Rev. Lett..
    • Measurement of the time-dependent $CP$ asymmetry in $B^0 \to J/\psi K^0_{\rm S}$ decays, http://arxiv.org/abs/1211.6093, Phys. Lett. B.
    • First evidence of the $B^0_s \to \mu^+\mu^-$ decay, http://arxiv.org/abs/1211.2674, Phys. Rev. Lett..
    • First observation of the decays $\bar{B}^0_{(s)}\to D_s^+K^-\pi^+\pi^-$ and $\bar{B}^0_s\to D_{s1}(2536)^+\pi^-$, http://arxiv.org/abs/1211.1541, Phys. Rev. D.
    • A study of the $Z$ production cross-section in $pp$ collisions at $\sqrt{s}$ = 7 TeV using tau final states, http://arxiv.org/abs/1210.6289, J. High Energy Physics.
    • Measurement of the $B^0$--$\bar B^0$ oscillation frequency $\Delta m_d$ with the decays $B^0 \to D^- \pi^+$ and $B^0 \to J\ \psi K^{*0}$, http://arxiv.org/abs/1210.6750, Phys. Lett. B.
    • Observation of $D^0 - \overline{D}^0$ oscillations, http://arxiv.org/abs/1211.1230, Phys. Rev. Lett..
    • First observation of the decay $B^+ \to \pi^+ \mu^+\mu^-$, http://arxiv.org/abs/1210.2645, J. High Energy Phys..
    • Measurement of the $C\!P$ asymmetry in $B^0 \to K^{*0} \mu^+ \mu^-$ decays, http://arxiv.org/abs/1210.4492, Phys. Rev. Lett..
    • Measurement of the $D^\pm$ production asymmetry in 7 TeV $pp$ collisions, http://arxiv.org/abs/1210.4112, Phys. Lett. B.
    • Evidence for the decay $B^0 \to J/\psi \omega$ and measurement of the relative branching fractions of $B^0_s$ meson decays to $J/\psi \eta$ and $J/\psi \eta'$, http://arxiv.org/abs/1210.2631, Nucl. Phys. B.
    • First evidence for the annihilation decay mode $B^{+} \to D_{s}^{+} \phi$, http://arxiv.org/abs/1210.1089, J. High Energy Phys..
    • Measurements of $B_c^+$ production and mass with the $B_c^+ \to J/\psi \pi^+$ decay, http://arxiv.org/abs/1209.5634, Phys. Rev. Lett., 109: 232001, 2012.
    • A model-independent Dalitz plot analysis of $B^\pm \to D K^\pm$ with $D \to K^0_{\rm S} h^+h^-$ ($h=\pi, K$) decays and constraints on the CKM angle $\gamma$, http://arxiv.org/abs/1209.5869, Phys. Lett. B, 718: 43-55, 2012.
    • Differential branching fraction and angular analysis of the $B^+ \to K^+ \mu^+ \mu^-$ decay, http://arxiv.org/abs/1209.4284, J. High Energy Phys..
    • Search for the rare decay $K_{\rm\scriptscriptstyle S}^0\rightarrow\mu^{+}\mu^{-}$, http://arxiv.org/abs/1209.4029, J. High Energy Phys..
    • Measurement of the fraction of $\Upsilon(1S)$ originating from $\chi_b(1P)$ decays in $pp$ collisions at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1209.0282, J. High Energy Phys., 11: 031, 2012.
    • Measurement of the ratio of branching fractions $B(B^0 \to K^{\ast 0} \gamma) / B(B^0_s \to \phi \gamma)$ and the direct $C\!P$ asymmetry in $B^0 \to K^{\ast 0} \gamma$, http://arxiv.org/abs/1209.0313, Nucl. Phys. B, 867: 1-18, 2012.
    • Measurement of the $B^0_s \rightarrow J/\psi \bar{K}^{*0}$ branching fraction and angular amplitudes, http://arxiv.org/abs/1208.0738, Phys. Rev. D, 86: 071102, 2012.
    • Observation of $B^0 \to \bar{D}^0 K^+ K^-$ and evidence of $B^0_s \to \bar{D}^0 K^+ K^-$, http://arxiv.org/abs/1207.5991, Phys. Rev. Lett., 109: 131801, 2012.
    • Measurement of the effective $B_s^0 \to K^+ K^-$ lifetime, http://arxiv.org/abs/1207.5993, Phys. Lett. B, 716: 393-400, 2012.
    • Study of $D_{sJ}$ decays to $D^+K^0_{\rm S}$ and $D^0K^+$ final states in $pp$ collisions, http://arxiv.org/abs/1207.6016, J. High Energy Phys., 10: 151, 2012.
    • Measurement of the $\bar{B}^0_s$ effective lifetime in the $J/\psi f_0(980)$ final state, http://arxiv.org/abs/1207.0878, Phys. Rev. Lett., 109: 152002, 2012.
    • Measurement of prompt hadron production ratios in $pp$ collisions at $\sqrt{s} = $ 0.9 and 7 TeV, http://arxiv.org/abs/1206.5160, Eur. Phys. J. C, 72: 2168, 2012.
    • Measurement of $b$-hadron branching fractions for two-body decays into charmless charged hadrons, http://arxiv.org/abs/1206.2794, J. High Energy Phys., 10: 037, 2012.
    • Observation of excited $\Lambda^0_b$ baryons, http://arxiv.org/abs/1205.3452, Phys. Rev. Lett., 109: 172003, 2012.
    • Observation of double charm production involving open charm in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1205.0975, J. High Energy Phys., 06: 141, 2012.
    • Measurement of the $B_s^0\to J/\psi K_S^0$ branching fraction, http://arxiv.org/abs/1205.0934, Phys. Lett. B.
    • Measurement of relative branching fractions of B decays to $\psi(2S)$ and $J/\psi$ mesons, http://arxiv.org/abs/1205.0918, Eur. Phys. J. C.
    • Measurement of the $D_s^+ - D_s^-$ production asymmetry in 7 TeV pp collisions, http://arxiv.org/abs/1205.0897, Phys. Lett. B, 713: 186-195, 2012.
    • Measurement of the isospin asymmetry in $B \to K^{(*)}\mu^+ \mu^-$ decays, http://arxiv.org/abs/1205.3422, J. High Energy Phys., 07: 133, 2012.
    • Measurement of the CP-violating phase $\phi_s$ in $\overline{B}^0_s \to J/\psi\pi^+\pi^-$ decays, http://arxiv.org/abs/1204.5675, Phys. Lett. B.
    • Analysis of the resonant components in $\overline{B}^0_s \to J/\psi\pi^+\pi^-$, http://arxiv.org/abs/1204.5643, Phys. Rev. D.
    • Measurement of the branching fractions of the decays $B_s^0 \rightarrow D_s^\mp K^\pm$ and $B_s^0 \rightarrow D_s^- \pi^+$, http://arxiv.org/abs/1204.1237, J. High Energy Phys..
    • Measurement of the ratio of prompt $\chi_{c}$ to $J/\psi$ production in $pp$ collisions at $\sqrt{s}=7$ TeV, http://arxiv.org/abs/1204.1462, Phys. Lett. B, 718: 431-440, 2012.
    • First observation of decay $B_c^+\to J/\psi \pi^+\pi^-\pi^+$, http://arxiv.org/abs/1204.0079, Phys. Rev. Lett..
    • Measurement of the polarization amplitudes and triple product asymmetries in the $B_s^0 \to \phi\phi$ decay, http://arxiv.org/abs/1204.2813, Phys. Lett. B, 713: 369-377, 2012.
    • Inclusive $W$ and $Z$ production in the forward region at $\sqrt{s}$ = 7 TeV, http://arxiv.org/abs/1204.1620, J. High Energy Phys..
    • Measurement of $\psi$(2S) meson production in pp collisions at $\sqrt{s}$=7 TeV, http://arxiv.org/abs/1204.1258, Eur. Phys. J. C, 72: 2100, 2012.
    • Strong constraints on the rare decays $B^0_s \to \mu^+ \mu^-$ and $B^0 \to \mu^+ \mu^-$, http://arxiv.org/abs/1203.4493, Phys. Rev. Lett., 108: 231801, 2012.
    • Observation of $C\!P$ violation in $B^\pm \to D K^\pm$ decays, http://arxiv.org/abs/1203.3662, Phys. Lett. B.
    • Measurements of the branching fractions and $C\!P$ asymmetries of $B^{\pm} \to J\!/\!\psi\, \pi^{\pm}$ and $B^{\pm} \to \psi(2S) \pi^{\pm}$ decays, http://arxiv.org/abs/1203.3592, Phys. Rev. D, 85: 091105(R), 2012.
    • Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s} = 7$ TeV, http://arxiv.org/abs/1202.6579, Eur. Phys. J. C, 72: 2025, 2012.
    • Measurement of the ratio of branching fractions ${\cal B}(B^0 \to K^{\ast 0} \gamma)/{\cal B}(B^0_s \to \phi \gamma)$, http://arxiv.org/abs/1202.6267, Phys. Rev. D, 85: 112013, 2012.
    • First evidence of direct $C\!P$ violation in charmless two-body decays of $B^0_s$ mesons, http://arxiv.org/abs/1202.6251, Phys. Rev. Lett., 108: 201601, 2012.
    • Opposite-side flavour tagging of $B$ mesons at the LHCb experiment, http://arxiv.org/abs/1202.4979, Eur. Phys. J. C, 72: 2022, 2012.
    • Measurement of the $B^\pm$ production cross-section in $pp$ collisions at $\sqrt{s}=7$ TeV, http://arxiv.org/abs/1202.4812, J. High Energy Phys., 04: 093, 2012.
    • Search for the $X(4140)$ state in $B^+\to J/\psi\phi K^+$ decays, http://arxiv.org/abs/1202.5087, Phys. Rev. D, 85: 091103, 2012.
    • Determination of the sign of the decay width difference in the $B^0_s$ system, http://arxiv.org/abs/1202.4717, Phys. Rev. Lett., 108: 241801, 2012.
    • Measurement of the cross-section ratio $\sigma(\chi_{c2})/\sigma(\chi_{c1})$ for prompt $\chi_c$ production at $\sqrt{s}=7$ TeV, http://arxiv.org/abs/1202.1080, Phys. Lett. B, 714: 215-223, 2012.
    • Searches for Majorana neutrinos in $B^-$ decays, http://arxiv.org/abs/1201.5600, Phys. Rev. D, 85: 112004, 2012.
    • First observation of the decays $\overline{B}^0 \to D^+ K^- \pi^+ \pi^-$ and $B^- \to D^0 K^- \pi^+ \pi^-$, http://arxiv.org/abs/1201.4402, Phys. Rev. Lett., 108: 161801, 2012.
    • Observation of X(3872) production in $pp$ collisions at $\sqrt{s}=7$ TeV, http://arxiv.org/abs/1112.5310, Eur. Phys. J. C, 72: 1972, 2012.
    • Measurement of $b$-hadron masses, http://arxiv.org/abs/1112.4896, Phys. Lett. B, 708: 241-248, 2012.
    • Observation of $\overline{B}^0_s \to J/\psi f'_2(1525)$ in $J/\psi K^+K^-$ final states, http://arxiv.org/abs/1112.4695, Phys. Rev. Lett., 108: 151801, 2012.
    • Measurement of mixing and CP violation parameters in two-body charm decays, http://arxiv.org/abs/1112.4698, J. High Energy Phys., 04: 129, 2012.
    • Measurement of the $B^0_s-\overline{B}^0_s$ oscillation frequency $\Delta m_s$ in $B^0_s \to D^-_s (3)\pi$ decays, http://arxiv.org/abs/1112.4311, Phys. Lett. B, 709: 177-184, 2012.
    • Measurement of charged particle multiplicities in $pp$ collisions at $\sqrt{s}$ = 7 TeV in the forward region, http://arxiv.org/abs/1112.4592, Eur. Phys. J. C, 72: 1947, 2012.
    • Differential branching fraction and angular analysis of the decay $B^{0} \rightarrow K^{*0} \mu^+ \mu^-$, http://arxiv.org/abs/1112.3515, Phys. Rev. Lett., 108: 181806, 2012.
    • Measurement of the CP-violating phase $\phi_s$ in the decay $B^{0}_s \to J/\psi \phi$, http://arxiv.org/abs/1112.3183, Phys. Rev. Lett., 108: 101803, 2012.
    • Measurement of the CP violating phase $\phi_s$ in $\overline{B}^0_s \to J/\psi f_0(980)$, http://arxiv.org/abs/1112.3056, Phys. Lett. B, 707: 497–505, 2012.

    LHCf

    • Measurement of forward neutral pion transverse momentum spectra for $\sqrt{s}$ = 7TeV proton-proton collisions at LHC, http://arxiv.org/abs/1205.4578, Phys. Rev. D.
    • Comparison of hadron interaction models with measurement of forward spectra by the LHCf apparatus, http://cdsweb.cern.ch/record/1434705, Nuovo Cimento C, 034: 135-140, 2011.
    • Measurement of zero degree inclusive photon energy spectra for $\sqrt{s}$= 900 GeV proton-proton collisions at LHC, http://arxiv.org/abs/1207.7183, Phys. Lett. B, 715: 298-303, 2012.

    TOTEM

    Saturday, December 08, 2012

    GRAIL's Gravity Tour of the Moon


    Embedded video from
    NASA Jet Propulsion Laboratory California Institute of Technology
    This movie shows the variations in the lunar gravity field as measured by NASA's Gravity Recovery and Interior Laboratory (GRAIL) during the primary mapping mission from March to May 2012.