and the phases of matter - Harvard Universityqpt.physics.harvard.edu/talks/unc16.pdfQuantum entanglement and the phases of matter University of North Carolina, Chapel Hill April 18,
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Metals without quasiparticles - Harvard Universityqpt.physics.harvard.edu/phys268/Lec11_Metals... · Logarithmic violation of “area law”: S E = 1 12 (k F P )ln(k F P ) for a circular
Superfluid-insulator transition - Harvard Universityqpt.physics.harvard.edu/talks/berkeley16.pdf · Mott insulator. The thin dashed lines are contours of consta nt ρ.Intheapplicationtothecuprate
Activity P55: Transistor Lab 1 The NPN Transistor as …mars.umhb.edu/~wgt/phys2412/Labs/P55.pdf · Physics Labs with Computers, Vol. 2 Student Workbook P55: Transistor Lab 1 - Digital
Quantum Phase Transitions - Harvard Universityqpt.physics.harvard.edu/c40.pdf · phase transitions, which are caused by the increasing importance of entropy in determining the phase
Quantum Phase Transitions - Harvard Universityqpt.physics.harvard.edu/c43.pdfQuantum Phase Transitions 5 These must be at least one point of non-analyticity as a function of g: for
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Quantum Entanglement, - Harvard Universityqpt.physics.harvard.edu/talks/simons17.pdfThe complex quantum entanglement in the strange metal does not allow for any quasiparticle excitations.
Andrea Allais and Subir Sachdev - Harvard Universityqpt.physics.harvard.edu/p265.pdf · 2015-10-10 · Spectral function of a localized fermion coupled to the Wilson-Fisher conformal
electrons in two dimensions - Harvard Universityqpt.physics.harvard.edu/c28.pdf · arXiv:cond-mat/0109419 v1 23 Sep 2001 Quantum phase transitions of correlated electrons in two dimensions
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Quantum vortices and competing orders - Harvard Universityqpt.physics.harvard.edu/talks/maryland.pdfmagnetic translation algebra 2 1 with 2 if xy yx MI TT e TT p f q π δ = − ==
Quantum Criticality - Harvard Universityqpt.physics.harvard.edu/talks/kac1.pdf · Talk online: sachdev.physics.harvard.edu S. Sachdev and B. Keimer, Physics Today, February 2011 Thursday,
Classical phase transitions - Harvard Universityqpt.physics.harvard.edu/phys268b/Lec1_Classical_field_theory.pdf · 3.2 Landau theory 41 Figure 3.1 Plot of (3.16) as function of N
Strange metals and black holes - Harvard Universityqpt.physics.harvard.edu/talks/kvpy_public17b.pdf · 10.12.2017 · National Science Camp (Vijyoshi) - 2017 Indian Institute of
Metallic spin glasses - Harvard Universityqpt.physics.harvard.edu/p71.pdf · spin glass and paramagnetic phases are metallic or insulating, as the e ective theory of spin uctuations
Bosons in tilted Mott insulators - Harvard Universityqpt.physics.harvard.edu/talks/yale11.pdf= quasi-particle = hole = quasi vacuum = = ∆ t −1 diagonal tilt: not all sites can
Abstract - Harvard Universityqpt.physics.harvard.edu/p268.pdf · 2015. 9. 27. · The random-mass is expected to be a relevant perturbation to the SDW quantum critical point of L,
