SCIENTIFIC ABSTRACT LANDAU, L. D. - LANDAU, L.

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• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

SUDAKOV, V.V.; UNDAU L.D., akademik.
4--,
IsotaDic-invariant theory of ~-decay. Dokl. AN SSSR 90 no.6:1009-1010
A 15~- (YJJIA 6.6)
1. Akademiya nauk SSSR (for Landau). (Nuclear physics)

SBICVBMV, Yaj.; LANDAU. L.D., akademik
Poiaeuille's flov in nonsymmetrical radial clearance; analogy vith the
torsion of beams. Dokl. AN SSSR 91 no.1:35-38 J1 '53. (MLRA 6:6)
1. Akademiya nauk SSSR (for Landau) (Fluid mechanics)

LIPSHITS, I.X.; XOSIVICH, A.M.; UNDAIJ, L.D., akademik.
On the theory of magnetic susceptibility of thin metal layers at low
temperatures. Dokl.AN SSSR 91 no.4:795-798 Ag 153. (MMA 6;8)
1. Akademiya nank SM (for landau). 2, Fiziko-tekhnicheskiy institut
Akademit nank Ukrainskoy SSR (for Lifshito and Kosevich). 3. Kharikov-
ski,y gosudarstvennyy universitet Im. A. M. Gorlkogo(for Lifshits and
Kosevich).
(Xagnetism) (Xetals at low temperatures)

AnIYEM, A.; A IN, V.; 1!!5L, . ., akademik.
'b
Magnetization time in!weak solution5 of He3 in He4. Dokl.AS SSSR 92 no.2:259-
262 S '53. ()aaA ':9)
1 0
1. Akademiya nauk SSSR (for landau). 2. l'isiko-tekhnicheakiy institut Akade-
mii nauk Ukrayinskoy SSR, Kharlkov (for Ak:hiyezer and Aleksin).
(Helium--Isotope,s) (Magnstim)

BIMTETSKIY, V.B.; LANDAU, L.D., akademik.
Decay into 37-mesona and the hypothesis of isotopic invariance. Dokl.As
SSSR 92 no.3:519-521 S 153- (MLHA 6.-9)
1. Akademiya nauk SSSH (for Landau). (Mesons) (Isotopes)

LANDAUP LO
B. T. R.
June 1954
Physics
,67760 Electron-AYA!amche Protes"s at Ul It
(Russian.) nd
~rnfl Nauk 4, hc?RJTwt9573-, lpu%9703'~S"
Inveligates rational processes under conditions in whicb theory
developed by Bethe and Heltler, of 'Irakf6g" radiation of
electrons ana positrons and of formatiQz) of electron-poslyon
Pairs by Y-quanta, Is incorrect. 2 r~f.

RUDNIK, A.; L"DAU, L.D., akademik.
Capture of mesons by-deuterons.
/k -
Dokl.AN SSSR 92 no.4:739-7L~2 0 '53.
(WTAA 6:9 ~
I -/
1. Akademiya nailk SSSR (for LaLndan). (Mesons) (Deuterons)

LIFSHITS, Ye-H.i AlEKS14YEV. D.K., redaktor; T-UPAUIM, N.A.,
. tekhnichaskiy redBktor
[HecbaaicB of continuouB media] Makhaniks sploahnykh sred. Izd.
2-oe, perer. i dop. Moskva, Goa. izd-vo teklmiko-teoret. lit.-ry,
1954. 795 p (KlaA 10:3)
Olla;ticlty) (Hydrodynamics)

001, its
eleavidynami',

AiAh6re &u 1'~ Do, Amlimudetmi Abrikosovi A. A. MuLlatnikov'I is us
ii~~c expressi.on of-the Green photon function in qwmtum

Wt. al eport,
A s of the Acad. of Scs.'of the USSR 951, 6,0 1177 - 11800
21 Apr 1954
Abstract i
-V)
'An:asymptotic expression-for the green photon function (D
I bid in quant= eltictrodynamica is derived. The article contains
a, djAwam.
s Acaoi.'of Sce. of the USSR

-$Ubci 1
tt"
. 25 Fab 1954

LAUAU, 1.D., skademik; '.KH&LATIIIKOV, I.M.
Anomalous absorption of sound near to the second-order phase transition.
Dokl.AN sssR 96 no..,1:469-472 my 154. (KLRA 7:6)
(Low temperature resemb) (Sound waves)

1%UMAU, Lev Davydovich; SMORODINSKIY, Yakov Abramovich; ALSKSEYKV, D.M.,
'V9 iij."16AVRILOV, S.S., i;ekhnicheBkiy redaktar.
[Lectures on the theory of the atomic nucleus] Lektsii pt tearii
atomnogo iadra. Moskva, Gos. izd-v-o tekhnike-teoret. lit-ry, 1955,
140 p. (Nuclear phraica) (KLRA 9:4)

J.
'Cexd:,
Pub 22- 16/60
aus Academician;- and Lifshits, R.7M.

ttitati` D UM

out:. thim, rotation of liqui h Ii

ke AN.. SUM 100/4 0'~I'Feb
46~472 1-:1955

i
Aw ex0lanation *of the isminar~r
'Struotdre of rotating he ium II liquid
M -tlie.thermodynamio~equalibriusi theory.
'10 given Ir the! of -vioiw of
ft~mdas 'are' derived for ~slcUaiting:~ the ~ thickness of the rotatizg.

1 rot,alions., ~'Four referencest I British'and
''k Vera for, fast and*a ow
3 11MR. -1951).
~(i941

ion.. j the S.- V..;7avilov Inatitute.of Phypical Problems
OrZas USM

.~A --~

LANDAU, L. D. , MIGDAL, A. B. and GALITSKIY I V. M.
"The Disintegration of the Deuteron by the Coulomb Field of the Nucleus" a paper
presented at the International Conference on Nuclear Reactions, Amsterdam, 2-7
July 1956.
D551274

L
L.D. -y-
r;
quanta
1"adiatiOr, Of CLL'-J,'
pions and I"uc:lei
jjccclcrat,,,-S and Piun
hys Ics
ceneva .11-2-1 Jlu',e
In. 'Brancl,

OF - - - - - - - - - - - - - - - - - - - - -- --------- -- ------ ---------- ----
USSR/Atomic and* Molecular Physics - Statistical Physics. Thermo- D-3
dynamics.
Abs Jour Ref Zhur - Fizika, Tio 4, 1957, 8973
Author Tands, L D
D
4_~~
Inst Otute oi Physical Problems, Academy of Sciences, USSR.
Title The Theory of a Fermi-Liquid
Orig Pub Zh. eksperim. i teor. fiziki, 1956, 30, No 6, 1058-lo64
Abstract A theory of a rermi liquid (FL) is developed, based an the
representation of the excitatJon energy as a functional of
the distribution function. In a Fermi gas (FG) with specified
(weak) interaction between the atoms at sufficiently low
temperatures the "indeterminacy of the momenta," connected
-with the finite length of the mean free path, - is alvays
small compardd with the! momentum itself, and with the width
of the Fermi smearing zone. This serves as the basis for
an assumption that as the interaction between the atoms Is
gradually "turned on-" i.e., upon transition from FG to a
FL, the classification of the levels remains unchanged. The
role of the gas particles in this classification is assuned
by the "elementary e='itations" ("qua6i-pafticles"), each of
which has a definite momentum. They obey the Fermi statistics,
Card 1/3

USSR/Atomic and Ylolecular Physics - Statistical Physics . Thermo- D-3
dynamics
Abs Jour -Ref Zhur - Fizika, 11o 4, 1957., No 8973
and their number agrees with the number of particles oT the
liquid. The variation of the energy density of the sy3tem
E is determined in the .9'nd _ is
form S E = sp,, Sc -r, where r
the energy of the quasi-particle, n the distribution fanction
of the quasi-particles, d?'the element of phase volume, and
Spa- is the trace over the spin states. Representing the
entropy of the FL in a combinatroial manner and using the or-
dinary supplementary conditioneS N = ~ E = 0, the autbor ob-
tains the Fermi distribution for the quasi-particles, n( E
exp Z-( E - 1
.,&)/6D7+ la , in which C- is a functional of
n. At low temperatures the F-L still obeys the linear law
for the specific heat. It differs from the specific heat of
the FG only in replacing the true masq m by an effective mass
of the quase-particle m* = 51( r)'E-M)PV~-~=po, where Po
is the limiting momentum of the Fermi distribution of the
quasi-particles at absolute zero. The change in 6 , caused
by the change -in n, is given by the expression C56 (p) :: Sp
a- - S C6E ) 6- '15C' . The function f can be considered as a
scattering amplitude of the scattering of.the quasi-jxLrticle
Card. 2/3

USSR/Atomic and Molecular Physics - Statistical Physics. Thermo- D-3
dynamics.
Abs Jour : Ref Zhur - Fizika, No 4, 1957, No 8973
by an angle 00 upon collision with each other, taken with
the negative sign. Using the Gal-lilean relativity principle,
a relation is obtained between m and ml. The compressibility
of the FL at absolute zero is computed. An expression is
obtained for the velocity of sound. The magnetic susceptibi.1-
ity of the FL is found to be 1/X := g -2 ~ 2.rr 2 K 2/3c4 + To I ,
where(3 is the magnetic moment of the free particlej>( the co-
efficient in the linear-law for specific heat, and tpo takes
into account the exchange interaction. An analysis of the
experimental results have shown that q)0 < 0 and amounts to
approximately 2/3 of the first term. Using the kinetic equa-
tions, the author obtains expressions for the momentum and
energy fluxes.
Card, 3/3

Ij ,oel--V V1r_
J
Landau, Lev Davydovich and Lifshits, Yevgeniy Mikhaylovich 203
Elektrodinam1ka sploshn-ylch sred (Electrodynamics of Continuous
Media) Moscow, Gostekhizdat, 1957. 532 p. (Uieir:
Teoreticheskaya fizika)
Ed: Rynik, V.I.; Tech. Ed: Murashova, N.Ya.
PURPOSE: This study is intended for advanced students and spe-
cialists with an excellent knowledge of mathematical
analysis and electrodynamics.
COVERAGE: The present volume of the "Theoretical Phys-.Tcs" series is
devoted to the theory of electromagnetic fields in material
media and to the theory of macroscopic electric and mag-
netic properties of matter. The authors consolidate, clarify,
and correct the literature existing on these theories. As in
the case of their classic Mekhanika sploshnyk ared (mechanics
of Continuous Media) they suggest in their investigation of
the phenomenaLof very diverse fields of science an integrated
approach which they think capable of fruitful. applications.
Personalities mentioned Ir-clude: Ginzberg, V.L,., Professor,
who contributed many valuable suggestions and ead the manu-
script; Dzyaloshinakiy, I.Ye. , and Pitayevskiy, L.P., who
Card '.L/9 assisted in proofreading. There are no references.

Electrodynamics Of C)ntinuous Media (Conte,) 203
TABLE OF CONTENTS:
Foreword 9
Symbols 10
Ch, 1, Electrostatics of Conductors 11
1. The electrostatic field of conductors
2. Energy of the electrostatic field of
conductors
3. Methods of solving problems in electrostatics 21
4. The conductive ellipsoid 36
5. Forces acting on a conductor 4,8
Ch. IL Electrostatics of T)ielectries 55
6. Electrostatic field in dielectrics 55
7. Dielectric pent~trability 57
8. Dielectric ellipsoid 62
9* Pielectric penetrability of a mixture 67
10. Thermodynamic relationship of dielectrics
in an electric field 69
11. Total free energy of the dielectric body 75
12. Electrostriction of isotropic dielectrics 79
Card s)/a

Electrodynamics of G-n.'~-;1nuous Media (Cont.)
13. Dielectric properties of crystals 83
14. Positiveness of dieleaL-nz,- susceptibility 88
15, Electrical forces in liquid dielectrics 90
16. Electrical for,-~es in solid bodies 96
17. Piezoelectric substances 2.02
18, Thermodynamic inequality lio
19. Seignetto-electric properties 114
Ch. III. Direct Current 125
20. Current density and conductance 125
21. Hall effect 130
22. Contact difference of potentials 133
23. Galvanic cells 136
24. Electrocapillarity 138
25. Thermoelectrical phenomena 140
26. Electrical diffusion phenomena 147
Ch, IV. Direct Magnetic Fields 150
2~. Direct magnetic field 150
28. Magnetic symmetry of crystals 154
29. Direct-current magnetic fields 158
'30. Thermodynamic relationship in a magnetic
r
0 ard 3/9 f ie ld- 7
I.A

Electrodynamics of 0;,~,mt-Lnuous Media (Cont 2 0 31

31.
Total f.L--e energy of magnetc, I
32. Current-system energy
33- Self-induction of linear conductors 17-
34. Power in a magnetic field 184-
35. Hydromagnetio phenomena -L8 -j
Ch. V. Ferromagnetism iao
36. P;~rromagneti~,. material close to the Gu:~ie
point 190
37. Energy of magnetic anisotropy 10-1
I ;
38. Magnetostriction of ferromagnetic materia-1s 20
39. Domain structure of ferxnmagnetic materials 20.5
40. Antiferromagnetic Curie p3int 213
Ch. VI. Sup erconductivity 215
41. Magnetic properties of superconductors 2-1-
42. Superconductive current 218
43. Critical fieldq 223
4-4. Intermediate oondition 228
Card 4/9

203
Electrodynamics of C-l"Atinuous Media (Cont.)
Ch. VII. Quasi-stationaxy electromagnetic fields 237
45. Foucault current 237
46. Skin effect 248
4?. Complex resistance 251
48. Capacity of a quasi-stationary current 256
49. Conductor movement in a magnetic field 261
50. Current excitation by acceleration 266
Ch. VIII. Magnetic Hydrodynamics 270
51. Equations of liquid movement in a
magnetic field 2?0
52. Magnetohydrodynamic waves 276
53. Tangential and rotating breaks 283
54, Shock waves 290
55. Spontaneous magnetic field during the
turbulent flow of a liquid conductor 296
Ch. IX. Eauations for Electromagnetic Waves 303
5 . Dielectric field equations in the absence
of dispersion 303
Card 5/9

2032
ElectrodynamiGs of rontinuous Media (Cont.)
5?. Electrodynamics of mobile dielectrics 308
58. Dispersion of dielectric penetration 314
59. I?ielec-'Jric penetration at very high
frequencies 317
60. Dispersion of magnetic penetration 318
61. Field of enerU-in dispersive media 320
62. Relationship between material and
imiaginary particles E60) 32-4.
63. Plane monor-h-romatic w4v,~6 333
64. Transparent media. 538
Ph. X. Propagation of Electromagnetic Waves 342
65. Geometric~ optics 342
66. Wave reflection and refraction 346
67. Surface J.mpedance of metals 354
68. Wave propagation in a nonuniform medium 361
69. Reciprocity theorem 365
70o Electromagnetic fluctations in hollow-
Card 6/9 space oscillators 368

Electrodynamics of Continuous Media (Cont.) 203
71. Diffusion of electromagnetic waves in
waveguides 372
72. Electromagnetic wave scattering on
small particles 379
?3. Absorption of electromagnetic waves
on small particles 384
74o Diffraction on a tapering surface 385
75. Diffraction on a flat screen 390
Ch. XI. Electromagnetic Waves in Anisotropic Media 395
76. Dielectric penetration of crystals 395
77. Plane wave in an anisotropic medium 397
78. Optical properties of uniaxial crystals 405
79. Biaxial crystals 408
80. Double refraction in an electrical field 414
81. Dvnamo-optical phenomena 415
82. Magneto-optical effects 417
83. Spontaneous optical activity 425
Ch, XII, M.'ansmission of Fast-Moving Particles
Tbrough Matter 433
84. Ionization losses of fast particles in
Card 7/9 matter., A case of non-relatiViBtiC 1088 433

Electrodynamics of Continuous Media (Cont.) 203
85. Ionization losses of fast particles in
matter. Relativistic oc-curence 439
86. Cherenkov radiation 448
Ch. XIII. Electromagnetic Fluctuatiozis 451
87. General theory of quantum fluctuations
of single, value 451
88. General theory of quantum fluctuations of
several values 459
89. Current fluctuations in linear chains 465
90. Fluctuations in an electromagnetic field 466
91. Black radiation in a transparent medium 473
92. Forces of molecular adhesion between
solid bodies 475
Ch. XIV. Scattering of Electromagnetic Waves 483
93. General theory of scattering in isotropic
media 483
94. Principle of detailed equilibrium in
scattering 491
Card 8/9
Electrodynamics Of Continuous Media (Cont.) 203
95. Scaftering.iiith low frequency change 494
96. Rayleigh scattering in gases and liquids 497
97, Critical opalescence 504
98. Scattering in amorphous solid bodies 506
Ch. XV. Diffraction of -X--Rays in Crystals 510
99. General theory of diffraction of x-rays 510
100. Integral intensitZ~ 517
101. Diffused thermal s,;attering of x-rays 520
524
Appendix. Curvilinear Coordinates
526
Index
AVAILABLE: Library of Congress
Card 9/9

- -1 ., T

LANDAUt L.D., MMEIANCquy, yuat.
nRadiation of Gamma (quanta R.1ring the Collision of Fast Pions
and Nuclei," paper presented at CMIA Symposium, 1956, appearing in
Nuclear Instruments, No. 1, pp. 21-30, 1957

AUTHOR LANDAU L.D. PA - 3053
TITLE -Off--tKe -oonse`i~v-ation Theorems at Weak Interactions.
(0 zakonakh sokhraneniya pri slabykh vzaimodeystviyakh.-Ruscian)
PERIODICAL Atomnaia Energiia 1957, Vol -2, Nr 2, PP 405-406 (USSR)
Received: 5/1957 Reviewed: 7/195*1
ABSTRACT First of all the paper under review points out the difficulties
which result for modern theoretical physics from the properties
of the K- mesons. As a matter of fact, the theoretical physicist
faces the following dilemma; either there exist two different
kinds of K-mesons, or the conservation theorems are no more
valid at the decay of K-mesons.
To assume the existence of two different kinds of K-mesona would
mean to contradict the experimental results, and thereforo there
remains only the popsibility that at K-decay the at present
assumed convorvation theorems are no more valid. As it is impo2-
sible to doubt the conservation of momentum, we have heret a direct
violat!Lon of the conservation theorem of parity. One could assume
that at weak interactions theoonseryation theorem of parity and
the inyariance are not valid in detail with regard to the charge
aonJugability. But it would be possible that there exists an
invariante with regard to the totality of the two operations
denoted as combined inversion in the paper under review). At such
CARD 1/2

On the Conservation Theorems at Weak Interactions.
J?A - 305 3
a combined inversion we have simultaneously a space inTersion
and a. transition of the particles into the corresponding anti-
particles. The invariance of all interactions with xegard to
a combined inversion leaves the total symmetiy of the space
unchanged. But the electric charges then prove to te asymme-
Trioal. In this case there results for charged particles no
conservation theorem of parity, because the operator of the
combined inversion does not transmit the charged particles into
themselves. Furthermore, the constants whioh characterize the
particles and antiparticles (massp life span) must be identical.
The really neutral particles, i.e. such particles whioh are
identical with their antiparticles, go over into themselves at
a combined inversion. For such particles the combined inversion
has the character of a normal spaoe inversions and for such
particles the conversation theorem of parity is valid at all
interactions.
(No reproductions)
ASSOCIATION: Ini4titute for Problems of Physics, Aeademy of Sciences of the USIM
PRESENTED BY: -
SUBMITTED: 11.12. 1956.
AVAILABLE: Library of Congress.
CARD 2/2

RIVOAU) L. J~>.
SpOscilution's of a Fermi FlU4 by L. D. lAndau, Tmg-t1tute of
Pbysical 2roblems, Academy of Sciences USSR, Zhurnallk~ ner
mentallnoy i Teoreticheskoy Aziki) Vol 32p No 1, JW1 57)
PP 59-66
"The present article presents an investigation of wave propagation in.
a Fermi fluid. The development is based on the general theory of such fluids
developed by the author (ZMT, 30, 1058, 1956). The phenomenon =at be
lLighly unusual in a Fermf -fluid since it is impossible fcr ordinary hydro-
Oiamic sound waves to propagate in it at absolute zero temperature. This
is obvious from the fact that path length and, with it, viscosity of a Fermi
.~lfluid tend to infinity as T~4 0. As a result, the coefficient of sound
miWorption increases without limit.
"It appears, however, that other waves, of a substantially different
nature from ordinary sound waves, can be propagated In a Fermi fluid at
absolute zero. We shall call such waves zero round, vares...."
Oscillations of a Fermi f1iiid at absolute zero and at temperatures
,above abs6lute.,zero, absorption of waves, and spin waves are discussed. (U)

AUTHOR LANDAU, L.D.,
TITLE Un the POS-311-1-rity for the
(Ob odnoy vozmozhnosti dlya
PERIODICAL Zhurnal Eksperim. i Teoret.
pp 40-4oB, (u.s.s.R.)
Received 5/1957
PA - 2715
Polarization Properties of the Neutrino.
polariiatsionnykh svo'ystv hey-trino , Russian)
Fiziki, 1957, Vol 32, Hr 2,
Reviewed 6/1957
ABSTRh'#T Tf we abandon the law of conservation of parity we obtain new proper-
ties of the neutrino. The Dirac equation for particle,s with the mass
zero is decomposed into two pairs of equations which are not connec-
ted with each other. If we limit ourselves to combined inversion, it
is possible to describe the neutrino with just one pair of equations.
According to the usual scheme this means that the neutrino is always
polarized only in the direction of motion (or in the opposite direction)
The antineutrino is always polarized in the corresponding opposite di-
r6ction. The author of the present paper denotes such a neutrino as
longitudinally polarized neutrino or, for short, as longitudinal neu-
trino. The mass of this longitudinal neutrino automatically equals zero,
and this is not changed by any kind of interaction. Tile concept of the
longitudinal neutrino considerablydiminishes the number of the possible
types of operators for weak interactions. In the paper, under review,
the author deals with decay of a myon into an electron and two neutri-
nos. As usual, the interaction operator isrepresented in the form of
a product of operators. The one operator is made up of the Y-operators
Card 1/2 of theInvon and of the electron,, whereas the other operator consists
T-

Dii the Possibility for the Polarization Properties of the Pk - 2715
Neutrino.
of the &
"r -operators of the two neutr-nos. For a longitudinal-neutrino
on]ly one combination, namely a scalar, can be composed of the tro
OPETators. Two combinations can be composed of myon and electron, na-
mely a scalsr and a pseudoscalar combination. When the decay of a myon
res-alts in a neutrino and an antineut-rino, oray a four-dimensional
vector can be composed from the operators of the longitudinal neutrino
and the longitudinal antineutrino. The experiments oh the decay of
myons do not contradict the conceptof the longitudinal neutrino and
they show clearly that at the decay of a myon we obtain a ntutrino
and an antineutrino. Finally the paper under review discusses the in-
fluence of longitudinality of the neutrino on the P-decay.
(No reproduction).
ASSOCIATION Institute for Physical Problems, Academy of Sciences of the USSR.
PMENTED BY
SUBMITTED -.1-1-12-1956
AVAILABLE Library-of Congress
Card 2/2

AWHOM LANDAU I.D LIFSHITStE.M. FA - 2990
TITLEs Hydrodynamic Fluctuations. (0 gidrodinamicheskikh fluktuatsiyakht
RIL-3 a ian)
PERIODIGALt Zhurnal Ilksperim.,j Teoret. Fiziki, 1957, Vol 32, Nr 3, pp 618-6ig
(U.S.S.R.)
Reoeived: 6 / 1957 Reviewed: 7 / 1957
ABSTRACTt Tho general Theory of hydrodynamic fluctuations can bke constructed
by the introduction of additional "foreign" terms into the equations
of motion of the liquid. (Similar to the method used by RYTOV for
fluctuations of the electromagnetic field in continuous media by
the introduction of corresponding "foreign fields",into the
MAXWELL equations).
The introduction of such additional terms can be realized by
various equivalent methods. The greatest advantage, however, is offer-
ed by such a form in whiah the fluctuations of the "foreign quanti-
tiea" in the various points of the liquid are not correlated with
each other. This is obtained by the introduction of a "foreign
volitage teasor" 8into the equation by WAVIER-STOKES and of a
Teotor of the "foitign heat current" ? into the equa-tion of heat
traviefer. (The.oontinuity equation remains unchanged). The system
of bydrodynamic equations then takes the following forms
Card 1/3

On Hydrodynamic -?Iuctuations. PA - 12990
aq/alb + dir(Q"r) O,Qav-i/at + -a Q/axi + adik/aY
Q7((i)s/at +7bs) (1/2)a;k("V"k + a,;k/ax,) - diT-q, q - -RaT + g.
/axk) + (aV. axi) - (2/3)6 avl/axl) +f (arl/axl) s
"i'k a %71 V ik 6ik + ik
The denotationa are here the same as those in the authors' well-
known textbook. Relations have yet to be added to these equationa, whi
deteMine the average value of the products of the components s ik
and gi.
The authors do so, at first assuming the fluctuations to be elassioal
and the viBoosity and heat conductivity of the liquid as being not
dispersing.
For~the velocity of the modification of the total entropy S of the
liquid the following expression applies
CT I av a ,~r,
f ik i k awTr
r
37-, 'T.
S 2T 17~ + ) - r7 1 dV
Card 2/3 The final formulae have the following formt

On Hydrodynamic Yluctuations PA - 2990
__3' 2kT 6 + 6 6 2
'r r -q/3) ] 6
ik( 10 tl)alm( 2't2) ii km im kl) 2
_> 2kT 2 6 6(
6(t 2 -t 1)gi(r1-tl)gk( r 2't2) e_ ik r2 r1 2
gj(r~'-tj)8lm(r .t
1 2 2) - 0
These results can easily be generalized for the asse in which a
dispersion of the viscosity coefficient ot the thermal conductivity
coefficient exists or that the fluctuations are quantum-like.
ASSOCIATION: Institute for Physical Problems of the Academy of Science of the
U.S.S.R.
PRESENTED BYs
SUBMITTEDt 29.11-1956
IVAILABLEs Library of Congress
Card 3/3

LAIMALU, L. D.) and LMHI'IS,, Ye. M.
Quantum Mechanics, lion-Relativistic Theory, Vol. 3, Course of Theoretical
Physics, Translated from Russian, by J. B. Sykes and J. S. Bell. 5151;1)-
Pergammon Press Ltd., England; for LZ and Canada, Addison Wesley Puhl. Co., 2w.
Reading Mass, 1958.

24 PHASE I BOOK EXPLOITATION SOV/1787
Landau, Lev Davydovichjand Yevgeniy Mikhaylovich Lifshits
Mekhanika (mechanics) Moscow, Fizmatgiz, 1958. 206 p. (Series:
Teoreticheskaya fizika, t. 1) 35,000 copies printed.
Ed.: B.L. Livshits; Tech. Ed.: S.N. Akhlamov.
PURPOSE: This book may be useful to engineers, scientific research
workers, and vuz students in the field of mechanics.
COVEY._!G'E: The book is the first volume of the new edition of the
authorst Theoretical Physics. The book discusses equations of
motion and their integration, impact of particles, vibrations
about a position of stable equilibrium, motion of a rigid bodyj
and canonical equations. The succeeding volumes will be: 2) The
Theory of the Field, 3) Quantum Mechanics (Nonrelativistic Theory),
4) Relativistic Quantum Theory, 5 Statistical Physics, 6) Hydro-
dynamics, 7) Elasticity Theory, 8~ Electrodynamics of Continuous
Media, and 9) Physical Kinetics. The authors thank I.Ye. Dzya-
loshinskiy and L.P. Pitayevskiy. L. Pyatigorskiy is mentioned as
having contributed to this field. There are no references.
Card 1/5

Mechanics
TABLE OF CONTENTS:
Foreword
sov/1787
7
Ch. I. Equations of Motion 9
1. Generalized coordinites 9
2. The principle of least action 10
3. Galileo's principle of relativity 13
4. Lagrangian function of a free particles 15
5. Lagrangian function of a system of particles 17
Ch. II. Iaws of Conservation 23
6. Energy 23
7. Impulse 25
8. Center of inertia 27
9. Moment of impulse 29
10. Mechanical similitude 33
Ch. III. Integration of Equations of Motion 37
11. Motion with one degree of freedom (odnomernoye dvizheniye)37
12. Determination of potential energy from the period of
oscillation 40
Card 2/5

Mechanics
13. Reduced mass
14. Motion in a central field
15. Kepler's problem
Ch. IV. Impact of Particles
16. Decomposition of particles
1~, Elastic impact of particles
1 . Scattering of particles
19. Rutherford's equation
20. Scattering at small angles
Ch. V. Small Vibrations [About a position of stable
21. Free vibrations with one degree of freedom
22. Forced vibrations
23. Vibrations of system with many degrees of fr
24. Vibrations of molecules
25. Damped vibrations
26. Forced vibrations in the presence of friction
27. Parametric resonance
SOV/1787
42
43
49
56
56
6o
64
70
73
equilibrium]76
76
so
edom 85
92
97
100
103
Card 3/5

Mechanics SOV/1787
28. Nonlinear vibrations log
29. Resonance in nonlinear vibrations 113
30. Motion in fast. oscillating field lig
Ch. VI. Motion of a Rigid Body 123
31. Angular velocity 123
32. Tensor of inertia 126
33. Moment of the impulse of a rigid body 135
34. Equations of motion of a rigid body 137
35. Euler's angles 140
36. Euler's equations 145
37. AbymetrIcal top 147
38. Contact of rigid bodies 155
39. Motion in noninertial reference system 160
Ch. VII. Canonical Equations 165
40. Hamilton's equations 165
41. Routhian function 167
42. Poisson's brackets 169
43. Action as a function of coordinates 173
44. Maupertuis principle 176
Card 4/5

Mechanics
45. Canonical transformations
46. Liouville's theorem
47. Hamilton-Jacobi equation
48. Separation of variables
49. Adiabatic invariants
50. General charcteristics of
of freedom
Index
AVAILABLEt Library of Congress
Card 5/5
Sov/1787
motion with many degrees
GO/ad
6-24-59
179
182
184
187
193
197
203

LMAU, LEV DAVYDOVICH
N15
613-053
J21
Statistical physics, by L. D. Landau and Ye. M. Lifshits
London., Paris, Pergamon Press; Reading, Mass., Addison-Wesley, 1958
484 P. Diagrs.
Original Russian title: Statisticheskaya Fizika (Teoreticheskaya Fizika., V.5)

LANDAUP L. D.
'Txcitations in Liquid Heliwa"
paper submitted, but not presented at the Yamerlingh Ormes Conference, Leiden,
Conference on Low Temperature Physics, leiden, 23-28 Jim 58.
Inst. for Physical Problems, AS 'USSR

AUTHORt Landau, L~D. Lcadc-mician "Ilc,occw~ 2 6. r" -
TITLE- The ~,aantlji-.-i Thec3-y Frcin Plar..~',, to thc Present Day (Tecriya
kvant ot Mlaksa Planka ~1.c z-,a.5hikh dney)
PERIODICAL! Priroda, lQr')B, Nr 10, PT) -21 ~-'jsn)
ABSTRACT: The autnor ae.~.!rib-s -~be of th6 q~aa.--Cumw thaory
from lla~- Piar-ck to DirF.,- an' in-~nt"4ons the o3cntributions, made
by Feyr,man, 3chviingei -Ird By 1954, Soviet thc-oreti-
clans had fcur;d a msar).~,, of avoid-irG the applioation Of the
peYtu--rbat2.cr,, t'~,eory - wi-~!~ su-rprising rzsult-s. After rigoir-
~U
cus calculati--311~ not ~rlv aye nc sensible reS-.1143 chtairied
but all inte--a,-,tiors ccm-Lletaly d4.~appear, The intensity of
all the calculated f:r,orq the theory, invariably
oome down to zoro, thus leavine the theory in a crisis,
Tends. tc. thro-., J:ubt C,'-. the DOint-ir)teraction concepts
Heiserbarg has tri~~-J f,-, the pasi few years to presurvc- the
poiz-vc -Int era;- tion, concert azid tc, inTZ'oiuce scme verry funj-a-
mental changes into the --foimal structure of the the--r,,T,.
Pertv--ba,~icn
Card 1/1

SOV/4-58-11-4/31
AUTHORS: Landau, L. D.,.Academician; and Rumer, Yu. B.,Professor
TITLE: Relativity of Time (Otnositellnost' vremeni)
PERIODICAL: Znaniye - sila, 1958, Nr 11, PP 4 - 6 (USSR)
ABSTRACTs On the basis of theories developed by Galilei, Michelson
and Einstein the authors demonstrate the relativity of move-
ment, time and 8pace. There are 7 drawings.
Card 1/1

I_j9fVD4 LAI
56-1-56/56
AUTHORt Landau, L. D.
TITLEt The Projerties of the Green Function of a Particle in Statistics
(Svoystva grinovskoy funktaii chastits v statistike)
PERIODICALt Zhurnal Eksperimentallnoy i Teoreticheskoy Fiziki, 1958, Vol. ~4t,
.Nr 1, pp. 262 - 264 (USSR)
ABSTRACTs The present report shows that certain very general relations can
be derived for the Green function G - -i of the par.
ticles. In this connection the indices 1 and ~ s9ow that the
T -operators are taken at the moments t 1 and t T is the symbol
of the chronological product and the averaging Kkes place over
the factual state of the given macroscopic system. Then formulas
for the chronological and for the spatial dependence of the ma-
trix elements of the operator W are given. The expressions for
the Green function are then transformed with the aid of these e3:-
pressions. Then follows the statistical averaging over the Gibbil
distribution. On that occasion the quantity G is expressed as a
function of the temperature T and of the chemical potential A.
Then the author goes over from the spatial-chronological repre-
Card 1/2 sentation of the Green function to its Fourier (Furlye) components,

56-1-56/56
The Properties of the Green Function of a Particle in Statistics
The expression for the Green function obtained after some further
steps of calculation is explicitly written down. A certain rela-
tion exists between the real part and the imaginary part of the
Green function. It is here explicitly written down for the case
of the Bose statistics and the Fermi statistics and specialized
for the case of the temperature zero.
ASSOCIATIONs Institute for Physical Problems AN USSR
(Institut fizicheskikh problem Akademii nauk SSSR)
SUBMITTEDi November 5, 1957
AVAILABLE;; Library of Con.-ress
Card 2/2

AUTHOR: Landaug L. D. SOV/56-35-1-13/59
TITLE: On the Theory of the Fermi Liquid (K teorii Fermi-zhidko.-ti)
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1958
Vol- 35, Nr 1, PP. 97 - 103 (USSR)
ABSTRACT: In connection with two previous papers by the same avithor
(Refs 1 and 2), which deal with the general theory of
the Fermi liquid$ the present paper investigates the
collision of quasiparticles in a Fermi liquid at
0
acattering angles of 0 . For the investigation of the
scattering properties of the quasiparticles, the author
lroceeds from the variation of the energy of the interacting
particles during a modification of their distribution
function:
(p) - Sp
(~F p
where dV = d3V/(2n)3 ands = 1. The function fa,pl) dealt
with in detail by reference 1 characterizes the scattering
amplitude of the quasiparticles in the liquid in collisions
Card 1/3 of quasiparticles. For the investigation of the multi-

On the Theory of the Fermi Liquid SOV/505-35- -1 -13/519
particle system the author used a method of the quantLm
field theory based upon the application of Green's (Grin)
function G and the "vertex part" T. The properties of
these two functions and their application to the problem
to be investigated are described as follows:In the case
that momentum and energy transfer tend towards zerov the
scattering amplitude at the collision of quasiparticles
will depend esoentially upon the boundary value of the
ratio between momentum transfer and energy transfer. In
conclusion, the question is investigated as to which
of these boundary values are connected with the energy
of the interacting quasiparticles with respect to the
general theory of the Fermi liquid (Refs 1,2). The author
finally, expresses his thanks to A.G.Migdal, who drew
his attention to the dependence of the scattering amplitude
upon the ratio colk, as well as to Ye.M.Lifshits and L.?,
Gor1kov for their discussion of his paper. There are 3
references,82of which are Soviet.
Card 2/3

On the Theory of the Fermi Liquid SOV/56-35-1--13/59
ASSOCIATION: Institut fizicheskikh problem AN SSSR(Institute for
Physical Problems)AS USSR)
SUBMITTED: February 5, 1958
Card 313

PHASE I BOOK EXPLOITATION
sov/3865
Landau, Lev Davydovich, Academician, and Yuriy Borisovicb Rumer, Professor
Chto takoye teoriya otnositellnosti (What is the Theory of Relativity?)
Moscow, Izd-vo "Sovetskaya Rossiya,," 1959. 61 p. 15,000 copies printA.-d.
Ed.: Yu.E. Berenson; Tech. Ed.: N.L. Yusifina.
PURPOSE: This booklet is intended. for the general reader interested in the theory
of relativity.
COVERAGE: The booklet is a popular presentation of the basic concepts of the
theory of relativity and their role in modern physics. Various physical
phenomena are explained in terms of the theory of relativity by using
examples from everyday experience. No personalities are mentioned. There
are no references.
TABLE OF CONIXM:
Preface
Card 1/4
What is the Theory of Relativity?
Ch. I. Relativity to Which We are Accustomed
Does every statement make sense?
Right and left
What is it now - day or night?
Who is bigger?
The relative seems absolute
The absolute seems relative
"Comon sense" attempts to protest
Ch. Il. Space is Relative
One ancl the B place or not
How does a body actually move?
Are al'I points of view of equal value?
Position of rest is found
The laboratory at a position of rest
Is the train moving?
Position of rest definitely lost
Law of inertia
Velocity is also relative
2
80V/3865
5
5
6
6
8
8
9
3-1
12
13
14
15
15
17
18
19
Card 2/4

What is the Theory of Relativity?
Ch. Ill. The Drama of Light
Light is not propagated instantaneously
Is it possible to change the speed of light?
Light and sound
Principle of the relativity of movement seems shaky
The "cosmic ethern
A difficult position is created
Experience must decide
Principle of relativity triumphs
Oat of the frying pan into the fire
Ch. IV. Time is Relative
Is there really any contradiction?
Let's take the train
"Comwn sense" put to shame
The fate of space befalls time
Science trluWhs
Speed has a limit
Earlier and later
card 3/4
sov/3865
20
20
21
22
2k
25
25
27
27
30
31
32
34
35
36
38

What is the Theory of Relativity? sov/3865
Ch. V. Clocks and Rulers are Capricious
I,--tls take the train once again 40
Clocks systematically lose time 42
IBM ti= machine 43
Jr.yuwney to a star 45
Ubjects shrink 48
Speeds are capricious 51
Ch. VIL, Work Changes Mass
Mass 54
Mass increases 55
How mich does a gram of light cost? 56
S-aming up 58
AVAUMLE: Library of Congress
Card 4/4, JA/cdw/mas
8-lo-6o

L A.' D;l
Lt--cturt,s on Tiic C~~.-:,-
I - I-- dins"
-Y -iorc
i~ev. Ed. 11:-w Ycr'~,, Pl-nw-i -~rtss,
vii, 108 D. Illur'.) Dia, Tl,;bl!~,,,.
TranslatcCl, T-11--Cl.-i tlj~. Rus,.7-inn:
Letkts-L! Fo Troi-11 jltc-,.,:lnc,-o Y,~,Jra.

TeV
T)Pvidov-! ch
'!"I I, i (I r-'-r'rI3rIrI4 C-S, 1,y m-, Lard, ~-i~ :1. 7 t,-
London, PeinFamon Fress, "eri,--Iing A(,;ri i son-~-'Ifasj ey
A
'Pub. no., !P59-
XII, 53r, d"ai7y's., ural.0-s. (Theore4-,ica-l Physics,
Vol.
Translated from the orif- T-'ckhanika
inal Ruszii an:
sploshrykh sr(~d. "oscow, 19'-.L-.
Pi"bliographical frotnot,,.-s.

24(5)
AUTHOR: Landau, L. D.
SOV/56-37-1-10/64
TITLE: On the Analytical Properties of Vertex Parts in the Quantum
Field Theory (0b analiticheskikh svoystvakhVeriih1nbzA& chastey
v kvantovoy teorli polya)
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1959,
Vol 37, Nr 10), pp 62-70 (USSR)
ABSTRACT:, Numerous papers have in recent years been written about dis-
persion relations, which express the'analytical properties
of the quantities of the quantum field theory. Recently it
was found on the basis of such works as those.by Karplus,
Nambu, Sommerfeld and Wichman (Refs 1-3) that.a.representation
of the distribution and the singular-ities-.of..the.vartex.-i)arts
is possible in form of a direct diagram represent&tion. The
opinion that diagrams are not sufficient is based upon a mis-
understanding. The representation of quantum.quantities of
the field goes beyond the scope of existing theories,..and
therefore an assumption is made in which.neither ?,-operators
nor the Hamiltonian are used. The diagram practice is there-
fore the only possibility when calculating the dispersion
Card 1/3 relations, and is in no way equivalent to the perturbation

SOV/56-37-1-10/64
On the Analytical Properties of Vertex Parts in the 0antum Yield Therry
theory, because in the latter the quantum particles are con-
sidered to be stable, irrespective of the question as to
whether they are "simple" or "composed". A generalization of
the present diagram techniques must also serve as a basis
.for future theories. For the detection of singularities the
diagrams are analyzed at their ends. When setting up the diagrams
it is possible that at every branch-point an unlimited number
of lines converge. By the rules actually in force a restrio-
tion is, hoveverp imposed: thus, it is not possible for an
odd number of pions to intersect at one point. All stable
particles with strong interactiorBmay figure as lines. The
lengths of the internal lines correapond to the masses. Particu-
lar properties occur in the scattering amplitude. The integrals
are functions which are coinectel in the lower and upper half
plane by the relation F(x ) = F W, or, in other words;
above and below the axis functions are analyzed which are
non-analytical continuations of each other and which have the
significance of a discontinuity. In the case of "foreign" half
planes the factors a, b may have arbitrary and arbitrarily
distributed singularities, which can not be determined at
Card 2/3 all on the basis of general consideration. (Representation of

SOV/56-37-1-10/64
On tha Analytical Properties of Vertex Parts in the Quantum Field-Theory
the scattering amplitude according to Feynman. a(z - ia) +
+ b(x - W), e.g. the well-known resonanae-in the scattering
of pions by nucleonal vhich has the.property of "foreign.'
half planes. Such properties may be determined from.a. theory,
which gives an explanation of the scattering.amplitude.. The
author finally thanks L. B. Okuniq A. P. Rudik-and Ya. A.
Smorodinskiy for their valuable remarks. 2here- are-1-5 Sigures
and 3 references.
ASSOCIATION: Institut fizichaskikh problem Akademii nauk SSSR
(Institute of Physical Problems of the Academy of Sciences,
USSR)
SUBMITTED: February 19) 1959 (initially) and April 7, 1959 (after revision)
Card 3/3

24 (0) Landau -D J
AUTHOR: L. SOV/5'1-68-3-10/11
TITLE: ---V~rfG~g Pauli (Deceased) (Vollfgang Pauli)
PERIODICAL: Uspekhi fizicheskikh nauk, 1959, Vol 6B, HT 3, PP 557-559 (USSR)
ABSTRACT: On the occasion of the death of the famous theoretical
physicist and holder of the Nobel Prize, Wolfgang Pauli, at
Mrich in December 1958, the Russian Academician L. D. Landau
in his necrology discussed the scientific work of the deceased
and his great importance for modern physics. A list of the most
important publications and books by the deceased is attached.
There are 1 figure and 13 reforenGeo.
Card 1/1

PHASE I BOOK EXPLOITATION SOV/4308
Landau, Lev Davydovich Academician,and Yevgenly Mikhaylovich
7rifshits, Professor
Teoriya polya (Field Theory). 3rd ed., rev. Moscow, Fizmatgiz,
1960. 400 P. (Series: Teoreticheskaya fizika, t. 2)
25,000 copies printed.
Ed.: U. Ya. Margulis; Tech. Ed.: S. N. Akhlamov.
PURPOSE: This book is intended for students at schools of
higher technical education.
COVERAGE: The book is the third revised edition of the second
volume in a series on theoretical physics. The series will
consist of the following nine volumes: 1) Mechanics, 2)
Field theory, 3) quantum mechanics (nQnrelativistic theory),
4~ Relativistic.quantum theory, 5) Statistical physics,
6 Hydrodynamics, 7) Theory of elasticity, 8) Electrodynamics
of continuous media, and 9) Physical kinetics. The present
volume deals with the theory of electromagnetic and gravita-
tional fields. The material is based on the special and
general theories of relativity and the equations are derived
Car&47~9_

LANDAU, Lev Davidovich
Blectrodynamics of Continuous Media, by L.D.
Landau and Ye. M. Lifshits. London, New Tork,
Pergamon Press, Reading,, Mass.., Addison-Wesley,
ig6o.
X, 417 p. diagrs. (Theoretical Physics, V. 8)
Translated from the original Russian: Elektrodi-
nami.ka Sploshnykh Sred., Moscow., 1,059.
Bibliographical footnotes.

LANDAU, Lev Davidovich
Mechanics,by L.D. Landau and Te.M. Lifshits. New
York, Pergamon Press, Reading, Mass., Addison4lesley,
1960.
165 p. diagra (Course of Theoretical Physics,
Vol. 1)

LIM-AU, Lev Davidovich. akademik; RUIMR, Yuriy Borisovich, prof.
Figures which seem to be reassuring. I2obr.i rats. no.l:
17-18 Ja 16o. (Mla 13:4)
(Space flight)

88470
S/05 60/039/oo6/063/063
0 BoZW63
AUTHOR: Landau, L. D.
TITLE: Low Binding Energies in the quantum-field Theory
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1960,
Vol. 39, No. 6(12), pp. 1856-1857
TEXT: This "Letter to the Editor" shows that in the quantum-field theory
there is a relation between coupling constant and binding energy of
weakly bound but strongly interacting particles. A spin-zero particle c
(e.g.t a deuteron) is assumed to disintegrate into the particles a and b;
then M. = 11 + -1.1 where is the binding energy which is assumed t
c a ~b ov/~
be small. The particle c is supposed to be even with respect to the
spin-zero particles a and b (s-state). The total vertex part for the
a + b --~c transition is indicated by g. The mutual scattering amplitude of
particles a and b contains a pole-type term which is related to the virtual
production of particle c: (g2 +16 1" 2 _ M2 , or, if
a b) I (Pa+Pb) C3
Card 1/2

Low BindinJ Energies in the quantum-field
Theory
88470
S/056/6O/039/oo6/O63/o63
Boc)6/BO63
+ ' . + Z )2is substituted for (P 2 (E - rest energy in the center-of-
a 11b 2 2 a+Pb)*
mass system): (g /16n)/(M a+N ) (E +E) with small E and E . When conniparing
this exDression with that deriatLIDx-ibe resonance 8catterincy am...,litude,
2,
one obtains 32/16n(m +m )2 = J,,2 1 /"'4s+ 1 /Mb and, hence, ~ =(g"/5127-
a b
z,lso V. Faynberg and Ye. Fradkin obtained a similar relation
from the dispersion relations for nucleon scattering. There is 1 Soviet
reference.
ASSOCIATION: institut fizicheskikh problem Akademii nauk SSSR (Institute
of Physical Problems, Academy of Sciences USSR)
SUBLITTED: October 21, 1960
Card 212

LANDAU, L. D.
FME I BOOZ MI4MMM
Internaticnal Ccafermco ca HiGh-Encrey Physics* gth, Klyev, 1959.
Devyzatcya =:I~Mm=-caaqya Ix-afvamntoiVu po fiziLo vyzolzikh enorgly, Klyev
15-25 iyulya 1959 c:- (Ninth intermaticon, coaferance ca Rich-racra
Fh~micc_ Kiyov, July 15-23, 1959), Mo3cow, 1961. 739 j?. 2,500 coplea
printed.
Sp-oring A~--cy: Akid-zdya nailk S=. 11_,z~bauaarodW 807uz chjgtGV j
yrikladnoy fiziki.
Ccatributors not'=cuticned.
PJIUICSE: This b6dk Is Intended for nuclear pbysicists.
COMAC, * Me collectica cantalm 30 scj=tifie; articles pr,-rcntc& at tb* 9th
1hternation-al Ccafercnco cm 1110i-F_~ergy Physics, hold In Kiyev fr= 15 to
25 July 1959. Tho ar'~Iclcs rr,-sc;itcd relato mainly to tho prc,3r,,:;B,in nu-
clear pbyi3ics achieved in 1959. Subjects discussed aro the production of
Card 1/0

Ninth International Coaference (Coat.) 807/3982
nucleons, their structure, veak and strong interactions, scattering, and
their decay. No personalities are menticaed. References accompW 1ndi-
vidual articles.
TABIZ CP Cal-j=:
Opening or the Coarepence
334armardini, Go Photo;roiuatim of P14%ems and Compton Effect
cm Nucleons 11
Discussion 54
P(=tccorvo, B. Scattering of Pima bY Nucleons cad Single
Production of Pims :in lucloca-Nucleod and 60
Discussion 118
SogA, E. Antimelsona and Their Interactions 133
Discussica 152
Card 2/0 -22

Winth International Conferewe (Ccat.) SOV/5982
Shirkov, D. V. TheCretical Investigations of Dispersion Relaticns 453
Discussiob
465
Lebma=,, G. General Features of Transition Amplitudes and
h
Spectral Functions .69
Discussion
479
Schvinger, J. Field Theory of Unstable Particles 482
Discussion 507
Landau., L. ~D;eiOn Analytic Properties of Diagrams of
U)
~- um. Field Theory 512
t
Kaiar, A. A., M. A. Markov. On the Field Theory with
Green's Funatic" Having Hyperboloidal Singularities 516
Card. 5/ 8

LAEPAUI_Lev Davydovich, ekademik; LIFOUTS, Yevgeniy IUIchaylovich,
proT-.-j-TI7UMUU-S-,U.Ya.2 red.; AKHLAHOV, S.N.2 tekbn. red.
[Field theory] Teoriia polia. Izd.4-) ispr. i dop. Moskva,
Gon. izd-vo fizilio-inatem. lit-ry., 1962. 422 p. (Their Teore-
ticheskaia fizika, t.2.) (Field theory) (MIRA 15:3)
f
I

-- LANDAU, L.D.; RMIER, J.
Earth hour and rocket hour. Elet tud 17 no~45:1427-1428 1-1 N
1Q.

- LANDAU, Lev Davidovich, laureat Leninskoy i Nobelevskoy premiy
akademik; KITAYGOItODSKIY, Alekswndr isaakovich, prof.;
VERES, L.F., red.; GRIGOWVA, V.A., red.; KRYUGHKOA, V.!;.,
tekhn. red.
(Physics for all; motion heat] F-4zika dlia vsekh; dvizhenie,
teplota, Moskva, Fizmatgiz, 1963. 390 P. (14IRA 16:11)
(Physics)

LANDAU Lev Davydovich., akademik; LIFSHITS, Yevgeniy Mikhaylovich,
prof.; LIVSHITS, B.L., red.; PLAKSHE, L.Yu., tekhn.red.
[(quantum mechanics) Kvantovaia makhanika. lzd.!Z.p perer. i
dop. Moskvaq hzmatgiz. Vol.3. [Nonrelativistic theory]
Nereliativists~aia teoriia. 1963. 702 p. (MIRA 17:1)

IANDAU,, L.D., N,-,b&--'. d-iJ as
Ftndamental questiona.~ Fiz szende !'~ Jp- 763.
1 .1~
. I

LANDAU, Lev Davydovichp akademik; RUEER, Yuriy Borisovich, prof.y*
..- ~ .. ~ ICIMNIKOVA, M.S., red.; I-WAKASOVA, L.P., tekhn. red.
[What is the theory of relativity) Ghto takoe teoriia otno-
siteltnosti. 2. izd. Moskva, Sovetskaia. Rossiiap 1963. 73 p.
(MIRA 17:3)

LANDAU, Lev Davydovich, akademik; L-IFS3I!.'1T1-':', Y-evEyerdy Mit~hiyIrjvjch,
VIRKOY I.G., red.
[Statistical ph7jsics] Stathz!--4,~heskaia fiz--ka. I7-d.2.,. pe-
rer. MosIl-va, Imuka, 19c'..4. 56`7 p. (MIRA 18:1)

AH5023895 -JD/M'1/EM BOOK EXPLOITATION URI
531
'La ndau Lev Davidovi 4ifshita. YBv eni UMAYIPY-i-th
_tv~~Tsorotichesk
Theoreti6al~ physics,-, v, 71 Theory of 614stici aya
fizikao* to,7s Teoriya uprug6sti) 3d ado) rev. and enle Moscow$
Izd-vo "Naukal!., 1965. 202 p. illus., index* 67*000 copies printedo~
T.OPI'C TAGS: elasticity theory, elastic wave, dislocation, heat con-
::ductivityt viscosity
PURPOSE AND COVERAGE: This book is Volume 7 of a series "Theoretical!
Pliyeics" published by Izd-vo "Nauka". The theory of elasticity
is'presented as a separ,ate book in this third edition of the above
work* The precoding edition (1953) included hydrodynamics and
appeared under the title Makhatfika sploshnykh ared; (this book was
:-translated by,Jo Do Sykes and W. 11 Reid of the Pergamon Press under---
o on-W;sley Publishing Company, 1957).
the title Fluid Physics, Addis
The third edition contains a few relatively minor correction and
additions and.a new chapter on the microscopic theory of disloca-
tions. As tbis.book Is Intended.primarily for physicists, such
ILI-3-

,Section 290 Continuous distribution of dislocations -- 169
Section-,30*' Distribution of interacting dislocations -- 174

4,--akaderJk.-,. LIFSHITS, Yevgeniy Mikhaylovich,
~vDa~,d2yj-,
prof.; VLRKO, I.G... red.
[Mechanics] Mekhanika. Moskva, Na-aka, 1965. 203 P.
[Theory of elastic:ityl TecrLia uprugosti. Moskva, Nauka,
1965. 202 p.

LVIDAU)_J~y-.Pp~yyqovich (deceased]'- AKIIIYEZER, Aleksandr Illich;
~ -- N. J.
LIFSHITS, Yevgeniy 111i thaylovich; DUMOVA, V.Ya., red.
(General physics course; mechanics and molecular physics]
Kurs obshchei fiziki; mekhanika i molekuliarnaia fizika.
Moskva, Nauka, 1965. 384 p. (MI'lu 19:1)

LAMAV, L. G.
OSTRDVSKOGO* M. Ye.0 LANDAU, L. G. - Arkbitektor, ILIINSKIY, H. P. - Arkhitektor,
BAGUZOV, H. P. - Arkbitektor
Vaeso,vuznaya kontora tipovogo proyektirovaniya I tokhnicheskikb issle dovaniy
(KTIS) Mintyashatroya
Analiz proyektnykh reshenly proizvodstvennykh zdanly za 191+8-1949 gg. Page 65
SO: 2wlwt4= Ar AZbAt&tj= a pkiw-J-4,1r, Pagsnlncll-~ !"prk pr cpvstwJtlc,.n, CAM;~Lvud
IV 3S~5D. Ylosacm, 1951

r7 -t
UMU, L. G. arkhitektor.
Nev standard roofing components for industrial buildings. Stroi.
prom. 35 no-7:13-18 -11 157. (MIRA 10:10)
1. Gosudarstvennyy institu tipovogo proyektirovanniya i tekhnicheskikh
Iseledovaniy.
(Roofs)

LANDAU. L.G. itek-tor
Standardizing volumetrie planning and structural solutions for
industrial buildings and structures of by-product coke lants.
Str6f'. prom. 36 no. 7;20-26 J1 158. 7HIRA 11:8)
1, Giprotis.
(Coke ovens)
(Precast concrete construction)

(,_ LA.NUUk.-G, arkbitektor
Methods for improving the planning of standard Industrial con-
struction. Prom.stroi- 38 n0-3:22-27 16o. (HIRL 13:6)
1. GosudarstvenzW institut tipovogo proyektirovaniya I takhni-
cheskikh isoledovaniy.
(Factories-Design and construction)

.-LANDAUP-L.G., arkhitektor; VATMANp Ya. P.,, ark~itektor
Industrk6dde standardization is the basis of further improvement
in the assortment of precast reinforced concrete articles. Prom.
stroi. 39 no.4:46-48 161. (MIRA 34:6)
1. Moskovskiy institut tipovogo proyektirovani-ya i tekhnieeakikh
issledovani~y..
(Reinforced concrete-Standards)

BAGURZOVI H.P.j, arkhitektorpLANDAU, L.G., arkhitektor,- KATSMAN, D.S.,,
inzh.; WFAKOV, 1.4r-i=V. "
Range for using industrial buildings without montors. Prom.
stroi. 40 no-4:21-27 162. (MIRA 15;5)
(Factories-Design and construction)

VAT,.L,'N, Ya.:,'., L.G., arkhit.ektor
Problem-- in standurd sect-fons oil 1.1 -.,:: f , ~-,
.1 , c- .
Prom. itroj.. 42 nc.3:fS--!() 1 ~,5. (:,-~ IF:,I),
1. TSentra-I'vy i proyfAtno-ek:-,peri-
menta:lln3rj inst-Wit promimblennyx1h zdan'-y 1 sooruzhaMy.

-T,A NZ-)A2 U 1 11 ". 1 -1 t i "I
New sluand.!%rd
43 165o
menta-11r,vy instuiLut