Superfluidity and the Roton

University of Chicago scientists can create an exotic, particle-like excitation called a roton in superfluids with the tabletop apparatus pictured here. Posing left to right are graduate students Li-Chung Ha and Logan Clark, and Prof. Cheng Chin.

See: Cesium atoms shaken, not stirred, to create elusive excitation in superfluid 

We present experimental evidence showing that an interacting Bose condensate in a shaken optical lattice develops a roton-maxon excitation spectrum, a feature normally associated with superfluid helium. The roton-maxon feature originates from the double-well dispersion in the shaken lattice, and can be controlled by both the atomic interaction and the lattice modulation amplitude. We determine the excitation spectrum using Bragg spectroscopy and measure the critical velocity by dragging a weak speckle potential through the condensate—both techniques are based on a digital micromirror device. Our dispersion measurements are in good agreement with a modified Bogoliubov model. DOI: http://dx.doi.org/10.1103/PhysRevLett.114.055301

The Axion of the Quark Gluon Pasma?

In physics, an anomalon is a hypothetical type of nuclear matter that shows an anomalously large reactive cross section. They were first noticed in experimental runs in the early 1980s as short tracks in film emulsions or plastic leaf detectors connected to medium-energy particle accelerators. The direction of the tracks demonstrated that they were the results of reactions taking place within the accelerator targets, but they stopped so quickly in the detectors that no obvious explanation for their behavior could be offered. A flurry of theoretical explanations followed, but over time a series of follow-up experiments failed to find strong evidence for the anomalons, and active study of the topic largely ended by the late 1980s.

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Professor Emeritus Piyare L. Jain is a particle physicist at University at Buffalo. On December 6, 2006, he claimed discovery of the long-sought axion subatomic particle. ^[1]

The discovery involved Jain's use of 3-dimensional photographic medium targets in heavy-ion particle accelerators; modern detectors using electronic sensors were unable to detect the axion due to the very short distances and times involved, but the physical medium was able to identify about 1,200 Axion traces over years of experiment. Jain is one of the few currently working physicists with experience with that type of detector, which had been largely abandoned in favor of the modern electronic detectors.

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Axions, would also have stopped interaction with normal matter at a different moment than other more massive dark particles. The lingering effects of this difference could perhaps be calculated and observed astronomically. Axions may hold the key to the Solar Corona heating problem.[40] See: Axion

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Uploaded on Jan 9, 2011

SETI Archive: http://seti.org/talks

The Sun's outer atmosphere or corona is heated to millions of degrees, considerably hotter than its cool surface or photosphere. Explanations for this long-standing enigma typically invoke the deposition in the corona of non-thermal energy generated by the interplay of convection and magnetic fields. However, the exact physical mechanism driving coronal heating remains unknown. During the past few years, recently built instruments like the Japanese Hinode satellite, the Swedish Solar Telescope in Spain and NASA's Solar Dynamics Observatory (SDO) combined with advanced numerical simulations have revealed a new window into how the Sun's atmosphere is energized. These results directly challenge current theories and highlight the importance of the interface region between the photosphere and corona for understanding how the solar atmosphere is heated. Dr. De Pontieu will present some of these results and describe how NASA's recently selected Interface Region Imaging Spectrograph, which is being built by Lockheed Martin's Solar and Astrophysics Laboratory in Palo Alto, in collaboration with NASA Ames, Smithsonian Astrophysical Observatory (SAO), Montana State University, Stanford University and the University of Oslo, will be able to address many of the outstanding issues and problems.

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 An article on IAXO has been published in the September 2014 issue of the CERN Courier. You can see the online version of the article here (link is external), or dowload the full CERN Courier issue here (link is external).

The central component of iAXo is a superconducting toroid magnet. The detector relies on a high magnetic field distributed across a large volume to convert solar axions to detectable X-ray photons. The magnet’s figure of merit is proportional to the square of the product of magnetic field and length, multiplied by the cross-sectional area filled with the magnetic field.IAXO: the International Axion Observatory -Pg 9 Sept 2014(PDF)

Numerical Relativity and Consciousness

To model any process that as a BS(Belief System) system,  as in Numerical Relativity,  is to say that such computerization incorporates such photonic principles as to adhere to some aspect of the discovery of consciousness as a basis of that modelling?

The subsystem toward understanding consciousness is then the realization that such modeling is the outcome of projections into the basis of matter orientations. Intent,  as a force has move through such matters so as to gain in matter perspectives?

But if such an entry into such matter projections find significant "scientific value" then it is appropriate to say the understanding that the belief system has become part of the foundational constructive example of our orientations as a consequence? This is what is meant then by "to be lead by science," as a basic premise of understanding the beginnings of the truth with regard to understanding consciousness?

We build in matter? Numerical relativity is such an example. So where to from here?

Spintronics and orientation perhaps, so as to reveal some correspondence toward understanding the basis of the QGP?  This understanding not only with regard to the forward decay chain of this construct, but as a flowing straight through is but to reveal such a path with regard to the use of superconductors and its use in quantum computerization?

So we emulate consciousness you see?

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See Also:

• Numerical Relativity and Quantum Mechanics
• Materialism 

Numerical Relativity and Quantum Mechanics

Under normal conditions, quarks and gluons are confined in the protons and neutrons that make up everyday matter. But at high energy densities—the range accessible at today’s particle accelerators—quarks and gluons form a plasma reminiscent of the primordial Universe after the big bang. Understanding how the transition (Fig. 1) from the confined state to this quark-gluon plasma (and vice versa) occurs is a fundamental goal of experiments at the Relativistic Heavy Ion Collider and the Large Hadron Collider, which recreate the plasma by colliding nuclei at ultrarelativistic speeds. Theorists are therefore looking for new ways to study the transition with quantum chromodynamics (QCD), the mathematically challenging theory that describes the strong interaction between quarks. In Physical Review Letters, researchers in the HotQCD Collaboration report an analysis of this phase transition using a formulation of QCD that lends itself to numerical solutions on a computer, called lattice QCD [1]. Their simulations of deconfinement—the first to be performed with a version of lattice QCD that accurately describes the masses and, in particular, the symmetries of the quarks—yield the critical temperature for the transition to occur, and show that it is a smooth crossover, rather than an abrupt change.Viewpoint: Testing a Realistic Quark-Gluon Plasma  Bold and underlined added by me for emphasis

While the link(String theory may hold answers about quark-gluon plasma ) was shown in the previous post to this thread as numerical relativity it might be of difficulty that you persons respectively may be able to explain the nature of the connection,  if any,  between a relativistic interpretation with a quantum mechanical understanding? You understand it's a problem, how is it reconciled?

Record-breaking science applications have been run on the BG/Q, the first to cross 10 petaflops of sustained performance. The cosmology simulation framework HACC achieved almost 14 petaflops with a 3.6 trillion particle benchmark run,[51] while the Cardioid code,[52][53] which models the electrophysiology of the human heart, achieved nearly 12 petaflops with a near real-time simulation, both on Sequoia.Blue Gene

See also:

By using Einstein's equations to predict the pattern of gravity waves emitted during the collision of two black holes, or generated in a variety of other cataclysmic events, and comparing the predictions with the observations, an alliance of computational scientists from nine institutions plans to test this as yet unconfirmed prediction of Einstein's famous theory. These scientists belong to a research discipline called Numerical Relativity.

Numerical Relativity Code and Machine Timeline -

You may also find Feynman statement of some interest?

   As Richard Feynman put it:[13]

        "It always bothers me that, according to the laws as we understand them today, it takes a computing machine an infinite number of logical operations to figure out what goes on in no matter how tiny a region of space, and no matter how tiny a region of time. How can all that be going on in that tiny space? Why should it take an infinite amount of logic to figure out what one tiny piece of space/time is going to do? So I have often made the hypotheses that ultimately physics will not require a mathematical statement, that in the end the machinery will be revealed, and the laws will turn out to be simple, like the chequer board with all its apparent complexities".

Numerical simulations

Numerical simulations have different objectives depending on the nature of the task being simulated:

•  Reconstruct and understand known events (e.g., earthquake, tsunamis and other natural disasters).

• Predict future or unobserved situations (e.g., weather, sub-atomic particle behaviour).

Computational science -

So, Quantum Realism has to be looked at as a description of the real world? Does Quantum realism lead you to nothing? In context of the solution toward unification of Relativity and the quantum world is a "unification point?" Meaning......

An equilibrium point is hyperbolic if none of the eigenvalues have zero real part. If all eigenvalues have negative real part, the equilibrium is a stable equation. If at least one has a positive real part, the equilibrium is an unstable node. If at least one eigenvalue has negative real part and at least one has positive real part, the equilibrium is a saddle point. Equilibrium point -

That a straight line has to somehow be explained as not bending either one way or another and without losing information(even if information is scrambled)? Hopefully, you can help me here?

Perfect fluids are often used in general relativity to model idealized distributions of matter, such as in the interior of a star. Perfect fluid -

Then, A Theory in the Abstract

ALICE (A Large Ion Collider Experiment)Image Credit by CERN

Collisions in the LHC generate temperatures more than 100,000 times hotter than the centre of the Sun. For part of each year the LHC provides collisions between lead ions, recreating in the laboratory conditions similar to those just after the big bang. See: Alice

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You have to reach a certain point in which the experiments bring you to the question of what arises in the beginning and then update(See Susskind's Lecture 1: Theoretical Minimum.) So you figured out the time line here and saw that preceding this point in time there is a fundamental question about how the universe begins.

Your aware that the reductionist agenda has a dual purpose, to not only tell us about the matters at hand, but reveals something about the very nature of creation in the cosmos. All these satellites are sensor attributed to the spectrum allocations which we have given to in sensor design.   These satellites then track for us. They give us  information about what is evident as we examine  the cosmos. People for some reason have totally missed this point about sensor development and cosmos related journeys.You develop what you need too,  in order to examine exactly where we are living. Where you might one day hope to live? Rocks, become important because they may hold the value of what is needed while you are on that other planet or moon.

Why AMS given you can use the extended environment, or,  design experiments given the weightlessness of space?

It may be hoped given the encouragement I give my grandson(very subtle) that he will give himself to the physics with which my later life has occupied me. Its a tough thing even as a parent, or grandparent to see these children become the new generation( the choices we could have made at their age) with which they can now become what we are so fondly attached.

But you know the rules right,  about setting them free?:) At the same time,  I know something that is needed,  that he has, and if he chooses to "see further" then the experiment with which I can so easily shown above, then he will be able to venture further "if"  he chooses to go into the abstract. But given that he might be 1 of 100, does this mean we should stop updating?

Just maybe, you young physicists of the white cloak today, will some day meet your younger counterparts and say hello to my grandson.

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See Also:

• Detailed Characterization of Jets in Heavy Ion Collisions Using Jet Shapes and Jet Fragmentation Functions
• QGP Advances

Studying the Perfect Fluid

A simulated collision of lead ions, courtesy the ALICE experiment at CERN

A simulated collision of lead ions, courtesy the ALICE experiment at CERN - See more at: http://newscenter.lbl.gov/2010/11/04/lhc-lead/#sthash.yxm9loVb.dpuf

Within five different approaches to parton propagation and energy loss in dense matter, a phenomenological study of experimental data on suppression of large-pT single inclusive hadrons in heavy-ion collisions at both the BNL Relativistic Heavy Ion Collider (RHIC) and the CERN Large Hadron Collider (LHC) was carried out. The evolution of bulk medium used in the study for parton propagation was given by 2 + 1 dimensional or 3 + 1 dimensional hydrodynamic models which are also constrained by experimental data on bulk hadron spectra. Values for the jet transport parameter qˆ at the center of the most central heavy-ion collisions are extracted or calculated within each model, with parameters for the medium properties that are constrained by experimental data on the hadron suppression factor  See: Extracting the jet transport coefficient from jet quenching in high-energy heavy-ion collisions

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See Also:

• JET Collaboration Wiki

Freewill under Scrutiny

Photo courtesy of the Department of Rare Books and Special Collections, Princeton University Library.

 ΔpΔx ≥ h/2π

In contrast I seek to awaken a fair and good interpretation of the "I AM" as the intellect and, and about our choices.  How we make them, and how we can be mindful of them. So here in lies my understanding that, one's intellect must be in charge to refer to the one as sitting in a position not egotistically centered, but the ego in the "I am," egotistically centered.:) It can be Illusive as to pinpoint "the center." So God then,  is Symmetry, and Symmetry has been broken?

BEHOLDING beauty with the eye of the mind, he will be enabled to bring forth, not images of beauty, but realities, for he has hold not of an image but of a reality, and bringing forth and nourishing true virtue to become the friend of God and be immortal, if mortal man may. Would that be an ignoble life? PLATO

It is never easy to understand the full scope of the question of,  by belief alone. So I sought here to try and give this Free Will some foundation.

Whether a particular thing happens, says Aristotle, may depend on a series of causes that

"goes back to some starting-point, which does not go back to something else. This, therefore, will be the starting-point of the fortuitous, and nothing else is the cause of its generation." Metaphysics Book VI 1027b12-14) See: The Cogito Model

The direct action,  according to my understanding is that one has "gained from experience."  So experience, is in a way "a value system" which I may use in order to understand those choices,  as well as,  to use that "information" to make decisions. In this way, I have set the causal affect for the future as to a determination with which causal chains must be linked back too, this original position??

  Pierre Curie (1894): “Asymmetry is what creates a phenomenon.”

So with a place in mind, as the intellect, we see what transpires as we "project into the future." So then, as to set the course of action dependent upon, the theory behind the ability of Free Will. This becomes a determinant feature in the link as a causal that is no longer left too, happen stance.

I suspect that will, qualia, meaning and intentionality will turn out to be understood to be aspects of nature. But I suspect that by the time we have achieved this our understanding of nature will be quite different. That is, I suspect that we will only succeed in reducing minds to atoms when we have revolutionized our understanding of atoms in some way presently inconceivable.

I only have an intuition about the first step in this process, which is to bring time and the present moment-the now-into science and make it central to physics and prior to law. By embracing presentism and the openness of the future we radically recast the context for understanding what it means for anything-rock or atom or mind-to be part of nature. Lee Smolin

If we trace back this idea of Indeterminacy, what do we find? And how shall we find such an exchange as getting to the heart of the problem as to say, " it is quite wrong to try founding a theory on observable magnitudes alone. " Einstein goes on to say that it is the theory that decides what it is that we can observe.

"Possibly I did use this kind of reasoning," Einstein admitted, "but it is nonsense all the same. Perhaps I could put it more diplomatically by saying that it may be heuristically useful to keep in mind what one has actually observed. But on principle, it is quite wrong to try founding a theory on observable magnitudes alone. In reality the very opposite happens. It is the theory which decides what we can observe. You must appreciate that observation is a very complicated process. The phenomenon under observation produces certain events in our measuring apparatus. As a result, further processes take place in the apparatus, which eventually and by complicated paths produce sense impressions and help us to fix the effects in our consciousness. Along this whole path - from the phenomenon to its fixation in our consciousness — we must be able to tell how nature functions, must know the natural laws at least in practical terms, before we can claim to have observed anything at all. Only theory, that is, knowledge of natural laws, enables us to deduce the underlying phenomena from our sense impressions. When we claim that we can observe something new, we ought really to be saying that, although we are about to formulate new natural laws that do not agree with the old ones, we nevertheless assume that the existing laws — covering the whole path from the phenomenon to our consciousness—function in such a way that we can rely upon them and hence speak of'observations'...Physics and Beyond (pg67)

(bold added by me for emphasis)

In truest sensibility of the individual then is to seek some relation as to what by nature allows such observance in consciousness, so as to be able too, make decisions. Then, as too, "covering the whole path from the phenomenon to our consciousness—function in such a way that we can rely upon them and hence speak of 'observations'. " Any new theory then has to have had a foundation(causal chains) with which it can move forward and built upon that experience. While I truly speak to the process of science so as to demonstrate Einstein's wording and ways,  I am also speaking to the consciousness that uses this same information.

Laminar Flow

If symmetry is to have ever existed,  and,  you return to the original state, problems enter the picture because you are introducing "some thing" to the system? For example, you can only back up so far. The question is what does this fifth dimensional perspective allow you? You know Gravity and light have been joined?

Yes, when you change visual perspective, what does a line look like, as in viewing a cylindrical system, with such a viscosity?

You cannot show where droplets were injected, and to go beyond that point of submersion, an example of what begin in rotation would on reversibility, happen same. So, something is missing?

 My question is: could you ever learn the answer to an otherwise-intractable computational problem by jumping into a black hole?

Entanglement,  is not an option in such a system ? As is FTL, medium dependent? Changing viscosity rates show speed of light variance?

I want to discuss today reflect a different perspective: one that regards computation as no more “arbitrary” than other central concepts of mathematics, and indeed, as something that shows up even in contexts that seem incredibly remote from it, from the AdS/CFT correspondence to turbulent fluid flow. See:Recent papers by Susskind and Tao illustrate the long reach of computation

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Fluid Velocity Profile

Visualization above,  has specific destination in relation to specificity of drop,  as to show distance from center?

Kaluza-Klein theory is a model which unifies classical gravity and electromagnetism. It was discovered by the mathematician Theodor Kaluza that if general relativity is extended to a five-dimensional spacetime, the equations can be separated out into ordinary four-dimensional gravitation plus an extra set, which is equivalent to Maxwell's equations for the electromagnetic field, plus an extra scalar field known as the "dilaton". Oskar Klein proposed that the fourth spatial dimension is curled up with a very small radius, i.e. that a particle moving a short distance along that axis would return to where it began. The distance a particle can travel before reaching its initial position is said to be the size of the dimension. This, in fact, also gives rise to quantization of charge, as waves directed along a finite axis can only occupy discrete frequencies.

Kaluza-Klein theory can be extended to cover the other fundamental forces - namely, the weak and strong nuclear forces - but a straightforward approach, if done using an odd dimensional manifold runs into difficulties involving chirality. The problem is that all neutrinos appear to be left-handed, meaning that they are spinning in the direction of the fingers of the left hand when they are moving in the direction of the thumb. All anti-neutrinos appear to be right-handed. Somehow particle reactions are asymmetric when it comes to spin and it is not straightforward to build this into a Kaluza-Klein theory since the extra dimensions of physical space are symmetric with respect to left-hand spinning and r-hand spinning particles.

Also to further speculate.....

Oskar Klein proposed that the fourth spatial dimension is curled up in a circle of very small radius, i.e. that a particle moving a short distance along that axis would return to where it began. The distance a particle can travel before reaching its initial position is said to be the size of the dimension. This, in fact, also gives rise to quantization of charge, as waves directed along a finite axis can only occupy discrete frequencies. (This occurs because electromagnetism is a U(1) symmetry theory and U(1) is simply the group of rotations around a circle).

Placing comment here until approved  or not approved.

Instituting a experimental argument is necessary, when t comes to symmetry in the realtor of viscosity and entanglement? Light in Ftl is medium dependent?

This sets up analogue example of the question of firewalls as to imply Black holes and information?

Layman wondering.

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See also:

• Misconceptions that Lenny Susskind, Scott Aaronson may share
• Problems in Condensed Matter Physics and How String Theory Can Explain
• Quantum Mechanics and the Geometry of Spacetime 
• Gravitational Collapse and the Horizon

Symmetry Breaking and the Crab Nebula

The connection between superfluidity and symmetry breaking has had a glorious history. It has left us a rich legacy of fertile ideas, that seems far from exhaustion. PG 60 Superfluidity and Symmetry Breaking

You know while there have been processes unfolding with regard to supersymmetry, for the life of it,  I am having a hard time ever denying to myself that the result of any beginning had to have some emergent feature that arose from the very nature of the big bang itself.

So to then, one may see some signs in a biological sense,  as to the nature of evolution? So,  that all things can be defined in this way. But the issue then for me is how "information can exist, " so as to say that such a direction for that evolution,  as an emergent product,  must have some location with which such presence makes itself know(far left of the picture above)? Sure,  because of my ignorance, I would be asking how such information could have ever come into being so as to say that this universe is the one with which such expressions came to be, so I accept the universe as it is.

Click on image above and you create a larger view of a microscopic world

So to then,  for such a gap to exist.  I was most certainly thinking about the LHC's use with which such reductionism were being taken.  I was looking for such signatures as to wonder that if such a location is found then(QGP),  so we could say indeed,  the beginning of the universe, and the correlation drawn,  as to the ever reducibility pursuit as some relation to nature?

The Crab Nebula, created by a supernova seen nearly a thousand years ago, is one of the sky's most famous "star wrecks." For decades, most astronomers have regarded it as the steadiest beacon at X-ray energies, but data from orbiting observatories show unexpected variations. Since 2008, it has faded by 7 percent, activity likely tied to the environment around its central neutron star. (Video Credit: NASA's Goddard Space Flight Center)

Cosmologically it had to make sense too. So I  looked at events in the cosmos to help me understand what it is that was created in the moments we align ourselves too,as  in the LHC. While I looked at the picture(jet development and expression) above as to the timing with which such a environment, it is now reduced too, the Crab Nebula in its design. Would you deny the Crab Nebula had a previous showing with which the jets them self began to emerge?

An example then exists for me as to how such contributions that could arise in any nebula could have ever contributed to the way the universe is,  and if all such contributions taken to the same question,  helps to define the universe in ways that were preceded . Where that nature of the information is to reside.

So while we had found our limits with regard to Planck scale,  it is thought to me that such a symmetry had exist,  that all forms of that symmetry expresses itself as a forming dualistic nature,  for a symmetry breaking to exist,  and for such a division to take place from such a perfect place.

Energy Flow Without Impedance

It has always been of interest to me how one could get energy to flow quite freely without it succumb too the impurities that may have blocked that flow. I mean the correlation in my mind and being the layman that I am, could in itself demonstrate how my noise provided for the ability of someone not to seeing,  so as to just bungle up the message.

The development of superconductors that could be used in real-world applications, particularly power transmission, could transform the U.S. energy landscape. In addition to huge cost-savings, the higher capacity enabled by superconducting cables would help overcome urban power bottlenecks in today’s power grid, reducing the potential for blackouts and other power interruptions. It would also improve the cost-effective control of power flowing across the national grid and extend the operating life of existing high-load power lines. Furthermore, zero-loss transmission would enable the transfer of solar energy generated in parts of the U.S. where sunlight is most abundant to those where it is not, thus making other energy-saving technologies more practical and affordable. Complex Materials Unusual properties may lead to new superconductors

So I paragraph more those whose words who are not mine to see how the issues around that flow may be considered.. I must say a blog spot piece from Scientific American had got me thinking.

Photo Credit: “Superconducting wires by epitaxial grown on SSIFFS at Oak Ridge National Laboratory” taken on July 29, 2009 by the U.S. Department of Energy

 Photo Friday: Superconducting wires for long-distance electricity transmission By Melissa C. Lott

So to me I am always looking for processes that make energy flow in such a way, as to be correlated in the cosmos. I am looking for ways that energy can travel through and be described as cosmic particle collisions and subsequent, cosmic spallations that demonstrate the list of the ways in which this energy is being accounted for.

So it is important that the views we may of held in regard to how we see energy leak into unaccountability  had its day,  so as to see the current status of what is no longer counted as the missing energy any more.

Later studies and the investigation of much larger data samples have concluded that the event could not be ascribed to new physics but rather to some odd coincidence of detector effects and rare, but known, standard model processes. The Event From Another World

So what is left for me is this nagging feeling about what is explained as processes we do not quite understand and what we have always herald it as some inexplicable description of an unknown process. Herein,  it still remains a mystery and if you can move forward and make clearer the understanding of these processes in particle examinations then how much clear the impedance that such a mystery brings to our examination of the science behind these energy flows?

Of course these are materialistic version of ones grasp of the realities of things in the objective sense, but there is always more we can correlate in mind that we would have found such processes as similar in their expressions? So yes analogies also have to be most certainly clear as to those demonstrations as well.

The Least Resistance as Possible?

It is always of interest that communications over longer distances is made most capable and following an ole effect we see that where such tunneling allows such a process?

 Kapusta points out that the condensation temperature would be well below the cosmic background temperature, so it would be quite a feat to make this superfluid. However, Kapusta also notes that a sufficiently advanced civilization might use pulses of neutrino superfluid for long-distance communications.

On an abstract level how is one able to envision such a process unless such a hole provides for information to move through a center,  and information to move very fast.

Magnetism is a fundamental interaction shaping our physical world, at the basis of technologies such as magnetic recording or energy generation. Unlike electromagnetic waves, which can be routed and transmitted with waveguides to long distances, magnetic fields rapidly decay with distance. Here we present the concept, design, and properties of a magnetic hose which enables to transfer the static magnetic field generated by a source to an arbitrary distance, and along any given trajectory. We experimentally demonstrate the field transmission through the simplest hose realization using a superconducting shell with a magnetic core. We discuss possible application of magnetic hoses to harness quantum systems by addressable magnetic fields, in the context of quantum information processing.Magnetic hose: Routing and Long-distance Transportation of Magnetic Fields

See Also:

• Physicists Build World’s First “Magnetic Hose” For Transmitting Magnetic Fields
• SuperFluids
• The Right Spin for a Neutrino Superfluid

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

• A luminosity-independent measurement of the proton-proton total cross-section at sqrt(s) = 8 TeV, http://cdsweb.cern.ch/record/1495764, Phys. Rev. Lett..
• Luminosity-independent measurements of total, elastic and inelastic cross-sections at sqrt(s) = 7 TeV, http://cdsweb.cern.ch/record/1495761.
• Measurement of proton-proton inelastic scattering cross-section at sqrt(s)= 7 TeV, http://cdsweb.cern.ch/record/1495752.
• Measurement of proton-proton elastic scattering and total cross-section at $\sqrt{s}$ = 7 TeV, http://cdsweb.cern.ch/record/1472948.
• Measurement of the forward charged particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 7 TeV with the TOTEM experiment, http://arxiv.org/abs/1205.4105, EPL, 98: 31002, 2012.