@book{landau_theory_1995, series = {Landau and {{Lifshitz Course}} of {{Theoretical Physics}}}, title = {Theory of {{Elasticity}}}, author = {Landau, Lev Davidovich and Lifshitz, Eugin M and Berestetskii, VB and Pitaevskii, LP}, year = {1995}, keywords = {_tablet}, file = {/home/pants/.zotero/data/storage/AQ7G8AHB/Landau et al. - 1995 - Theory of Elasticity.pdf} } @article{fisher_specific_1990, title = {Specific Heat of {{URu}}{$_{2}$}{{Si}}{$_{2}$}: {{Effect}} of Pressure and Magnetic Field on the Magnetic and Superconducting Transitions}, volume = {163}, issn = {0921-4526}, shorttitle = {Specific Heat of {{URu2Si2}}}, abstract = {Specific heats were measured in the range 0.3 {$\leqslant$}T{$\leqslant$}30 K for 0{$\leqslant$}H{$\leqslant$}7T and P=0, and for H=0 and 0{$\leqslant$}P{$\leqslant$}6.3 kbar. For H=0 and P=0, the measurements were extended to 0.15K. Above the superconducting transition the H=0 and 7T data can be superimposed. For the magnetic transition near T0 = 18K, T0 increased with increasing P accompanied by a broadening and attenuation of the specific heat anomally. The superconducting transition near Tc = 1.5 K was broadened, attenuated and shifted to lower temperatures for both increasing P and H. The superconducting transition is similar to that of UPt3, and both the temperature dependence of the superconducting state specific heat and the derived parameters are consistent with an unconventional polar-type pairing.}, number = {1}, journal = {Physica B: Condensed Matter}, doi = {10/ck6dj9}, author = {Fisher, R. A. and Kim, S. and Wu, Y. and Phillips, N. E. and McElfresh, M. W. and Torikachvili, M. S. and Maple, M. B.}, month = apr, year = {1990}, pages = {419-423}, file = {/home/pants/.zotero/data/storage/HHVDKMSP/Fisher et al. - 1990 - Specific heat of URu2Si2 Effect of pressure and m.pdf} } @article{hornreich_lifshitz_1980, title = {The {{Lifshitz}} Point: {{Phase}} Diagrams and Critical Behavior}, volume = {15-18}, issn = {0304-8853}, shorttitle = {The {{Lifshitz}} Point}, abstract = {The Lifshitz multicritical point (LP) divides the phase diagram of a magnetic system into paramagnetic, uniform (ferro- or antiferromagnetic) and modulated (spiral or helicoidal) phases, which coexist at the LP. It can occur in a variety of different systems, including magnetic compounds and alloys, liquid crystals, charge-transfer salts, and structurally incommensurate materials. Theoretical studies, including renormalization group, exact spherical model and high temperature series expansion calculations, are reviewed with emphasis on possible experimental (including Monte Carlo) verifications of the theoretical predictions in three and two dimensional systems. Some promising materials for further research are indicated.}, journal = {Journal of Magnetism and Magnetic Materials}, doi = {10/ccgt88}, author = {Hornreich, R. M.}, month = jan, year = {1980}, pages = {387-392}, file = {/home/pants/.zotero/data/storage/FQWHY9TF/Hornreich - 1980 - The Lifshitz point Phase diagrams and critical be.pdf} } @article{lifshitz_theory_1942-1, title = {On the Theory of Phase Transitions of the Second Order {{II}}. {{Phase}} Transitions of the Second Order in Alloys}, volume = {6}, journal = {Proceedings of the USSR Academy of Sciences Journal of Physics}, author = {Lifshitz, EM}, year = {1942}, keywords = {⛔ No DOI found}, pages = {251}, file = {/home/pants/.zotero/data/storage/TAA9G46H/Lifshitz - 1942 - On the theory of phase transitions of the second o.pdf} } @article{lifshitz_theory_1942, title = {On the Theory of Phase Transitions of the Second Order {{I}}. {{Changes}} of the Elementary Cell of a Crystal in Phase Transitions of the Second Order}, volume = {6}, journal = {Proceedings of the USSR Academy of Sciences Journal of Physics}, author = {Lifshitz, EM}, year = {1942}, keywords = {⛔ No DOI found}, pages = {61}, file = {/home/pants/.zotero/data/storage/D9BYG3FK/Lifshitz - 1942 - On the theory of phase transitions of the second o.pdf} }