Spring 2008 colloquia:(colloquia already given are listed here):
| Apr 29 |
Stuart Freedman University of California at Berkeley |
Direct
Evidence of neutrino oscillations with KamLAND Experiments performed in the last ten years provide conclusive evidence that neutrinos are particles with mass and that the neutrino states that couple through the weak interaction are mixtures of mass eigenstates. KamLAND is a 1000 ton scintillation detector located deep underground in western Japan. KamLAND detects anti-neutrinos from Japanese nuclear reactors hundreds of kilometers away. The latest results provide the most direct confirmation that reactor anti-neutrinos oscillate between weak flavor states. KamLAND has also observed geo-neutrinos from radioactivity of the Earth. I will review the present understanding of neutrino mass and mixing in light of the latest results form KamLAND. |
Barbara Jacak |
| May 6 |
Laszlo Mihaly Kirean Boyle Jeremy Holt - Awards Colloquium Stony Brook |
Measurements of the Double Helicity
Asymmetry in Pion Production
in Proton Collisions at \sqrt s = 200 GeV and the Resulting Constraints on the Polarized Gluon
Distribution in the Proton Realistic Nuclear Interactions with Brown-Rho Scaling Medium Modifications |
Tom Weinacht |
Colloquia already given in academic
year 2007/2008:
| Date |
Speaker |
Title |
Local host |
| Sept 11 |
Peter Koch Department of Physics Stony Brook University |
Chair's colloquium Link to Slides |
|
| Sept 18 |
Abhay Deshpande Stony Brook University |
Proton
Spin Puzzle, Part II: The tale of the
elusive gluons... Movie of Presentation Exciting measurements leading to a new insight in to the gluon's role in determining the proton spin have now been released by the PHENIX Detector Collaboration at the Brookhaven National Laboratory. The measurements were made in 2005 and 2006 using polarized proton beams of the Relativistic Heavy Ion Collider (RHIC) colliding at 200 and 62.4 GeV in center of mass. I will present the new PHENIX results & their impact on our understanding of the nucleon spin. A discussion of their limitations will evolve in to an outlook on what's needed in near & far future to precisely understand the nucleon's spin structure. |
Tom Weinacht |
| Sept 25 |
Amber
Miller Columbia University |
Peeking
in Ancient Holes and
Seeking the Holy
Grail Movie
of Presentation |
Meigan Aronson |
| Oct. 2 | Peter Schiffer Penn State |
Fun in the Sand: Some Experiments
in Granular Physics Movie
of Presentation References: Physical Review Letters 82, 205 (1999); Physical Review Letters 84, 5122 (2000); Physical Review E 64, 031307 and 64, 061303 and 64, 061303 (2001); Physical Review Letters 89, 094301 (2002); Physical Review E 67, 051303 (2003); Nature 427, 503 (2004); Physical Review E 70, 041301 (2004); Nature 442, 257 (2006). |
Meigan Aronson |
| Oct. 9 | Ed Brown Michigan State University |
Journey
to the Core of
an Accreting Neutron Star Movie of Presentation A neutron star is born in our galaxy about once every century. These stars, composed of the densest matter in nature, have long fascinated astrophysicists. Many observed neutron stars accrete hydrogen- and helium-rich matter from a companion. During the slow compression to nuclear density the accreted matter is transmuted from being proton-rich to being proton-poor. These reactions produce and affect many observable phenomena - from energetic explosions on the neutron star's surface to the recently detected thermal relaxation of the surface layers - that in turn inform us about the nature of dense matter in the deep interior of the neutron star. In this talk I'll describe the journey of matter that is accreted onto a neutron star, highlight some recent exciting discoveries, and discuss what they are telling us about the inner workings of neutron stars. |
Mike Zingale |
| Oct. 16 | Drew Shindell Nasa, Goddard Institute for Space Studies |
Climate
Change: Causes,
Consequences & Solutions Movie of Presentation Changes in the Earth’s climate are driven by shifts in the balance between the planet’s incoming and outgoing radiation. I will compare climate change in the Earth’s past with the current warming, discussing the various drivers and feedbacks at work during these times. I will then discuss the global climate models used to interpret recent climate change, and present projections from these models of how the climate may change in the future. I will talk about the uncertainties in current knowledge, and the consequences associated with projected changes. In addition to global temperature changes, these include shifts in the hydrologic cycle, the frequency of extreme events, and rapid warming of the Arctic with implications for ice sheet stability and sea-level rise. Finally, I will outline some potential strategies for climate change mitigation. |
Tom Weinacht |
| Oct. 23 | Thomas
Weinacht Stony Brook |
Observing and
Controlling Atomic and
Molecular Dynamics Movie of Presentation Ultrafast laser pulses can be used to initiate and capture atomic and molecular motion in real time. Shaping these pulses allows us to control the dynamics we observe. I will discuss some experiments that follow bond breaking and formation driven by an ultrafast laser pulse. I will also discuss an experiment where a shaped ultrafast laser pulse is used to control lasing of an atomic ensemble. I will conclude with some future prospects and goals. |
Hal Metcalf |
| Oct. 30 | Paul
Brumer University of Toronto |
Quantum
Interference in the
Control of Molecular Processes Movie of Presentation Coherent Control offers a powerful approach to the control of atomic and molecular processes. By manipulating quantum interference effects, primarily through laser excitation, control over multipath molecular processes can be achieved. This lecture will provide an introductory overview of coherent control, followed by a summary of new developments in the control of both bound state and scattering processes. |
Tom Weinacht |
| Nov. 6 | Steve Howell NOAO |
Mass
Donor Stars in
Cataclysmic Variables Movie of Presentation Observations of the low-mass donor stars in cataclysmic variables have had a renaissance in recent years due to the availibility of large aperture telescopes such as Keck and the VLT. Optical and infrared spectroscopy of the faint donor stars have revealed that some are brown dwarf-like objects while others appear to be normal main sequence stars. This talk will review the current state of the data, compare and contrast with the accepted paradigm and theoritical models, and discuss a few specific, highly interesting stars. |
Mike Zingale |
| Nov. 13 | Pierre Meystre Optical Sciences Center, U of Arizona |
Cooling
of nanoscale mirrors Movie of Presentation The observation of quantum
dynamics in truly macroscopic objects appears increasingly feasible as
a result of recent experimental advances thatinclude novel cooling
techniques and progress in nanofabrication. This is an exciting
prospect, as it would enable us to explore the quantum-classical
boundary as well as to test quantum mechanics in an entirely new
regime. The implementation of characteristically quantum mechanical
phenomena at a macroscopic scale also promises technological benefits
for areas from quantum measurement to the interferometric detection of
gravitational waves and to atomic force microscopy.
A promising route to these objectives is through the use of optomechanical systems, particularly optical cavities where the support of one of the mirrors is a nanoscale cantilever. The talk will review recent developments in the optical cooling of these moving mirrors and discuss the prospects for reaching their quantum mechanical ground state of vibration. Future directions, including the realization of ro-vibrational quantum entanglement in these systems, will also be touched upon. |
Hal Metcalf |
| Nov. 27 | Gustaf Brooijmans Columbia University |
After
the Standard Model Movie of Presentation From a particle physics point of view, the past thirty years can rightfully be considered as the golden age of the standard model. Both the theoretical and experimental knowledge of the structure of the strong and electroweak interactions has reached impressive levels of precision, and the agreement between experimental results and theoretical predictions is stunning. The standard model doesn't tell us anything about the nature of the particles whose interactions it describes however. We hope that data taken at the LHC starting in 2008 will allow us to develop some understanding of the origin of particle properties. According to some models we will learn about particle masses through the discovery of the Higgs boson, while others suggest that dynamics in additional spatial dimensions might be the source of specific properties. This colloquium will review some key aspects of our current knowledge and how it was acquired, followed by some speculation about what might happen at the LHC. |
John Hobbs |
| Dec. 4 | Paul Chaikin NYU |
Experimental Geometry
Experiments with candies and colloids Movie of Presentation There are some problems in Physics/Mathematics which can't be solved analytically or computationally (yet). But we can get the answer experimentally. Packing problems, how densely objects can fill a volume, are among the most ancient and persistent problems in mathematics and science. For equal spheres, it has only recently been proved that the face-centered cubic lattice has the highest possible packing fraction f ~ 0.74. It is also well-known that the corresponding random (amorphous) packings have f ~0.64. The density of packings in lattice and amorphous forms is intimately related to the existence of liquid and crystal phases and is responsible for the melting transition. The simplest objects to study after spheres are squashed spheres - ellipsoids. Surprisingly we find that ellipsoids can randomly pack more densely; up to f ~0.68 - 0.71 for a shape close to that of M&M'sO Candies, and even approach f ~0.75 for general ellipsoids. Randomly packed ellipsoids can pack more densely than spheres pack in a crystal!. The higher density relates directly to the additional rotational degrees of freedom of the ellipsoids which in turn is related to the number of neighbors, Z, needed to confine a particle. Quasicrystals can have symmetries which are disallowed for conventionly crystals, amongst them icosahedral symmetry which is the most spherical of discrete symmetries. They might be great candidates for a material that would trap light by having gaps in all directions. But their bandstructure can't yet be calculated. So we built a cm scale Quasicrystal and measured its paroperties int he microwave range. We found that quasicrystals have Brillouin zones despite having a dense set of Bragg peaks, and they are indeed the best candidates for photonic bandgaps. |
Meigan Aronson |
| Jan. 29 |
National Synchrotron Light Source Dept, |
Biomineralization: probing
protein-mineral relationships
with a synchrotron |
Tom Weinacht |
| Feb 5 | Stanley Brodsky | The
AdS/CFT Correspondence and Novel Effects in QCD Movie of Presentation One of the most interesting recent advances in hadron physics has been the application of the AdS/CFT correspondence to quantum chromodynamics. Although QCD is not a conformally invariant field theory, one can nevertheless use the mathematical representation of the conformal group in five-dimensional anti-de Sitter space to construct an analytic first approximation to the theory. The resulting AdS/QCD model gives accurate predictions for hadron spectroscopy and a description of the quark structure of mesons and baryons which has scale invariance and dimensional counting at short distances, together with color confinement at large distances. In addition, one can compute the form of the frame-independent light-front bound-state wavefunctions, the fundamental nonperturbative entities which encode hadron properties and which allow the computation of hadronic scattering amplitudes. A number of novel applications of light-front wavefunctions to QCD phenomenology will also be discussed, such as color transparency, hidden color, intrinsic charm, sea-quark asymmetries, dijet diffraction, direct hard processes, and hadronic spin dynamics. |
George Sterman |
| Feb 12 | Sol Gruner | Putting the
Squeeze on Biology: Pressure Effects
on Macromolecules Movie of Presentation (Beginning is missing) Modest pressures encountered in the biosphere (i.e., below a few kbar) have extraordinary effects on biomembranes and proteins. These include pressure denaturation of proteins, as well as dramatic changes in monomer-multimer association, ligand binding, membrane ion transport, transcription/translation of proteins, virus infectivity, enzyme kinetics and conformational states. Yet all of the biomaterials involved are highly incompressible. The challenge is to understand the structural coupling between these effects and pressure to elucidate the relevant mechanisms. X-ray diffraction studies of membranes and proteins under pressure will be described. It is seen that the key is not the magnitude of the changes, but rather the differential compressibilities of different parts of the structure, leading to a biasing of conformational substates. Examples will be given of pressure studies on biomembranes and proteins. Lessons learned have important implications for the freezing of protein crystals, as is routinely done for protein crystallography and on the role or water in proteins. |
Tom Weinacht |
| Feb 19 | Hal Metcalf Stony Brook |
Entropy
Exchange in Laser Cooling Movie of Presentation Laser cooling is usually viewed as compression in velocity space by a velocity-dependent force but such forces do not conserve energy. A proper description must include the light field that absorbs the energy from spontaneous emission, so the light field must be part of the system. It is usually presumed that spontaneous emission is necessary to remove the entropy lost by the atoms, and a closer look suggests that this happens by redistributing the light among the empty states of the radiation field. But the laser beams themselves have sufficient entropy capacity so that stimulated emission can do precisely the same thing. Thus the system doesn’t undergo a loss of entropy but merely its redistribution among its parts of the system. The entropy in the light field is not dissipated until the outgoing beams hit the walls in a non-conservative, irreversible process. |
Tom Weinacht |
| Feb 26 | Martin Schmaltz Boston University |
New
Physics at the LHC, why and what? Movie of Presentation With the start of the Large Hadron Collider in 2008 particle physics is likely to enter its most exciting period in over three decades. The physics of the TeV scale will begin to be uncovered, and whatever is found will have profound implications for the field. In this talk I review the argument for why we expect to see new physics at the LHC and present one of the leading proposals for what this new physics might be. |
Gilad Perez |
| Mar 4 | Robert
Panoff Shodor Foundation |
Many-Body for
Anybody:
A Computational Science Exploration of the Physics of More Than One
Thing Movie of Presentation Computational science continues to advance the accurate description and prediction of the dynamics of many-body systems with new applications, algorithms, and architectures. Moving from the researcher's workbench to the classroom, real-time model solutions and simulations are now possible in most every area of education and research in physics. These interactive learning environments help us to understand complex systems, while opening up new areas of learner-centered, group-oriented, discovery-based learning. We will explore such simulation environments from atoms to galaxies. As we progress to petascale computing environments, the use of more complex numerical models of these systems demands a greater emphasis on the fundamentals of quantitative reasoning, computational thinking, and multiscale modeling with special attention to verification and validation: how do you know if it is right? |
Alan Calder |
| Mar 11 | Joe
Eberly Department of Physics and Astronomy, Univ. of Rochester |
Mysteries
of Quantum Entanglement Movie of Presentation The invention of the two-photon Clauser interferometer signalled a completely new domain of spectroscopy. It allowed direct experimental demonstration for the first time of non-local, non-realist phenomena in physics. I will describe an idealized version of this interferometer and various phenomena at the interface between classical and quantum physics that are related to it (e.g. Schroedinger's Cat). An indirect consequence is that decay to steady state is not always what we were taught. Recent experiments on photons and atoms demonstrate the difference between local decay and non-local decay of entangled quantum systems. Even when decay of a system is locally smoothly asymptotic, non-local entanglement may be non-smooth and disappear discontinuously. This "sudden death" constitutes a strongly counterintuitive trait of entanglement, confirming earlier predictions, but not yet really explained. |
Tom Weinacht |
| Mar 25 | Max Tegmark MIT |
New
clues about inflation, dark matter and dark energy Movie of Presentation With a cosmic flight simulator, we'll take a scenic journey through space and time. After exploring our local Galactic neighborhood, we'll travel back 13.7 billion years back to explore the Big Bang itself and how state-of-the-art measurements and new theoretical insights are transforming our understanding of our cosmic origin and ultimate fate. |
Gilad Perez |
| April 1 |
Delia Milliron Lawrence Berkeley National Laboratory |
Chemical routes to phase change memory materials Phase change memory technology, a leading candidate for future non-volatile memory, is based on switching small volumes of metal chalcogenide material between the amorphous and crystalline states. A key remaining concern is the power required to switch from the crystalline to the amorphous state, and optimized low power cell designs call for the phase change material to fill a tall narrow channel between the contact pads. I will describe our efforts to develop a chemical approach to prepare metal chalcogenide materials. Molecular precursors are synthesized, deposited by spin coating, then thermally decomposed. Precursors can be combined in solution to control the composition, and properties, of the final metal chalcogenide film. By depositing from solution, we can easily fill small and high-aspect ratio holes through capillary action to yield arrays of free-standing nanodots or fill channels for memory devices. The promise of phase change memory lies in its projected scaling to very high density. We are therefore also synthesizing sub-20 nm colloidal nanocrystals to fast-forward the technology road map and investigate the fundamentals of phase switching on the nanoscale. |
Tom Weinacht |
| Apr 8 | Yuval Grossman | CP
violation: A solved problem (?) Movie
of Presentation |
Gilad Perez |
| Apr 15 | David Charbonneau |
The Era of Comparative
Exoplanetology When extrasolar planets are observed to eclipse their parent stars, we are granted unprecedented access to their physical properties. It is only for these systems that we are permitted direct estimates of the planetary masses and radii, which in turn provide fundamental constraints on models of their physical structure. Furthermore, such planets afford the opportunity to study their atmospheres without the need to spatially isolate the light from the planet from that of the star. I will review the most recent results, and then describe a new observatory that will survey 2000 nearby low-mass stars with a sensitivity to detect rocky planets orbiting within their stellar habitable zones |
Mike Zingale |
| Apr 22 | Krishna
Rajagopal MIT |
Quark-Gluon
Plasma in QCD, at RHIC, and in String Theory Movie of Presentation The realization that the high temperature phase of QCD is quark-gluon plasma, with properties qualitatively distinct from those of the hadronic phase whose quasi-particles make up the quotidian world, goes back more than 30 years. Over that time, we have gained reliable insight into the thermodynamics of quark-gluon plasma at accessible temperatures from lattice QCD calculations, and we have understood much about its dynamics in the high temperature limit where it becomes weakly coupled. However, in the last five years experimental discoveries at the Relativistic Heavy Ion Collider have taught us that, at least at temperatures within a factor of two of that at which hadrons ionize, the dynamics of quark-gluon plasma is closer to the ideal liquid limit than to the ideal gas limit. These experimental data demand a theoretical understanding of the dynamics of strongly coupled quark-gluon plasma. Such calculations in QCD itself are in their infancy, but string theory provides us with robust tools for exactly this purpose, applicable to the quark-gluon plasmas of many QCD-like theories. I will describe some of the many new insights into the properties of strongly coupled plasma obtained recently from these AdS/CFT calculations. |
Tom Weinacht |
For upcoming colloquia, go here.