SPECIFIC HEAT OF THE SUPERCONDUCTING STATE

[1] [Anonymous], 1955, HDB PHYS

[2] BORN M, 1954, DYNAMICAL THEORY CRY, P174

[3] DIFFERENCE BETWEEN NORMAL AND SUPERCONDUCTING STATES OF A METAL [J]. PHYSICAL REVIEW, 1956, 103 (06): : 1693 - 1699

[4] CORAK, 1956, PHYS REV, V102, P656

[5] CORAK, 1956, 1955 C PHYS BASS TEM, P503

[6] ATOMIC HEATS OF NORMAL AND SUPERCONDUCTING TIN BETWEEN 1.2-DEGREES-K AND 4.5-DEGREES-K [J]. PHYSICAL REVIEW, 1956, 102 (03): : 662 - 666

[7] GOODMAN BB, 1956, 1955 C PHYS BASS TEM, P506

[8] LOCK, 1951, P CAMBRIDGE PHIL SOC, V47, P811

[9] Maxwell E., 1952, PHYS TODAY, V5, P14, DOI 10.1063/1.3067418

[10] EFFECT OF DEFECTS ON LATTICE VIBRATIONS - INTERACTION OF DEFECTS AND AN ANALOGY WITH MESON PAIR THEORY [J]. PHYSICAL REVIEW, 1956, 102 (01): : 72 - 84

[1] [Anonymous], 1955, HDB PHYS

[2] BORN M, 1954, DYNAMICAL THEORY CRY, P174

[3] DIFFERENCE BETWEEN NORMAL AND SUPERCONDUCTING STATES OF A METAL [J]. PHYSICAL REVIEW, 1956, 103 (06): : 1693 - 1699

[4] CORAK, 1956, PHYS REV, V102, P656

[5] CORAK, 1956, 1955 C PHYS BASS TEM, P503

[6] ATOMIC HEATS OF NORMAL AND SUPERCONDUCTING TIN BETWEEN 1.2-DEGREES-K AND 4.5-DEGREES-K [J]. PHYSICAL REVIEW, 1956, 102 (03): : 662 - 666

[7] GOODMAN BB, 1956, 1955 C PHYS BASS TEM, P506

[8] LOCK, 1951, P CAMBRIDGE PHIL SOC, V47, P811

[9] Maxwell E., 1952, PHYS TODAY, V5, P14, DOI 10.1063/1.3067418

[10] EFFECT OF DEFECTS ON LATTICE VIBRATIONS - INTERACTION OF DEFECTS AND AN ANALOGY WITH MESON PAIR THEORY [J]. PHYSICAL REVIEW, 1956, 102 (01): : 72 - 84