statistical-physics-part-1

By E. M. Lifshitz, L. Landau. 1958

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Citations in the corpus

Statistical error in particle simulations of hydrodynamic phenomena (2002, methodology): “Landau introduced fluctuations into the hydrodynamic equations by adding white noise terms to the stress tensor and heat flux [ 16 ] (in the spirit of Langevins theory of Brownian motion).”
On the origin of band-tails in kesterite (2017, unknown): “In addition, contrary to first order phase transition, second order phase transition like the Cu-Zn disorder do not lead to phase segregation [74,75].”
An introduction to the Ginzburg-Landau theory of phase transitions and nonequilibrium patterns (2014, unknown): “[3], and Ref.”
On the roughness of single- and bi-layer graphene membranes (2007, background): “This is o f particular significance in the view of theoretical arguments which show that 2D crystals should not exist [9-14].”
One-dimensional quantum liquids: Beyond the Luttinger liquid paradigm (2011, methodology): “ is proportional to V qImP 0(q;!)ReP 0(q;!). However, we showed that ImP 0(q;!) is proportional to the noninteracting DSF, so ImP 0(q;!) /[! ! (q)] contains a threshold. The Kramers-Kronig relation (Landau and Lifshitz, 1980) therefore predicts a logarithm in the real part, ReP 0(q;!) /lnf[! ! (q)]=”
Network science: A Review Focused on Tourism (2010, unknown): “In statistical physics, power laws are associated with phase transitions (Landau and Lifshitz 1980; Langton 1990) or with fractal and self-similarity characteristics (Komulainen 2004).”
The structure of suspended graphene sheets (2007, background): “The question whether a strictly 2D crystal can exist was first raised theoretically more than 70 years ago by Peierls [4,5] and Landau [6,7].”
Combining GW calculations with exact-exchange density-functional theory: an analysis of valence-band photoemission for compound semiconductors (2005, unknown): “8”
Anomalies in thickness measurements of graphene and few layer graphite crystals by tapping mode atomic force microscopy (2008, background): “successfully identified graphene [2] and other 2D crystals [3] in a simple tabletop experiment, it was assumed that 2D crystals were thermodynamically unstable and could not exist under ambient conditions [4, 5].”
Analogue Gravity (2005, result): “At this stage some observations are in order: —(1) It is interesting to recognize that the dispersion relation (228) is exactly in agreement with that found in 1947 by Bogoliubov [36] (reprinted in [309]; see also [243]) for the collective excitations of a homogeneous Bose gas in the limit T → 0 (al”
Inhomogeneous superconductivity in condensed matter and QCD (2003, methodology): “To compute the free energy we make use of the theorem saying that, for small variations of an external parameter of the system, all the thermodynamical quantities vary in the same way (Landau and Lifshitz, 1996).”