Errata

(1)

HAL Id: jpa-00210176

https://hal.archives-ouvertes.fr/jpa-00210176

Submitted on 1 Jan 1986

HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

Errata - Longitudinal electronic and nuclear spin difference in atomic hydrogen

J.P. Bouchaud, C. Lhuillier

To cite this version:

J.P. Bouchaud, C. Lhuillier. Errata - Longitudinal electronic and nuclear spin difference in atomic

hydrogen. Journal de Physique, 1986, 47 (1), pp.145-145. �10.1051/jphys:01986004701014500�. �jpa-

00210176�

(2)

Longitudinal electronic and nuclear spin ^difference

in atomic hydrogen

J. P. Bouchaud and C. Lhuillier J. Physique ⁴⁶ (1985) ^1335-1344

One should notice that the collision integrals ^W given ⁱⁿ figure ² ^{and table} ^I differ from those defined and used in the text and appendix ^II by

^a

^factor

In figure ⁴ ^the quantity drawn is in fact n/k when k is the characteristic wavevector of the diffusion problem.

There is

a

factor 2 7r between the nL quantity defined in (22) and that drawn in figure ^4.

Structural study ^{of the} charge density ^wave phase transition of the blue bronze :

K0.3MoO3

J.-P. Pouget, ^C. Noguera, ^{A. H.} Moudden and R. Moret J. Physique ⁴⁶ (1985) ^1731-1742.

1. The X-ray ^diffuse scattering intensity reported in section 3. 2 (see ^for example that shown in figure 5) ^{has been}

measured

as

the extra scattering ^{above the} background. ^{Thus it} ^cannot ^be accounted for by ^the equation :

which gives

^an

absolute value of the diffuse intensity, ^without ^reference ^to ^the background ^With

^a

background

contribution of kT In 2 co’, corresponding ^to the response of the unstable lattice mode in the absence of its coupling

with the electron _gas, the measured diffuse intensity ^is actually given by :

where Y(q) ^is proportional ^to ^{the CDW} response function :

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphys:01986004701014500

Errata - Longitudinal electronic and nuclear spin difference in atomic hydrogen

HAL Id: jpa-00210176

https://hal.archives-ouvertes.fr/jpa-00210176

Submitted on 1 Jan 1986

HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

Errata - Longitudinal electronic and nuclear spin difference in atomic hydrogen

J.P. Bouchaud, C. Lhuillier

To cite this version:

J.P. Bouchaud, C. Lhuillier. Errata - Longitudinal electronic and nuclear spin difference in atomic

hydrogen. Journal de Physique, 1986, 47 (1), pp.145-145. �10.1051/jphys:01986004701014500�. �jpa-

00210176�

ERRATA

Longitudinal electronic and nuclear spin difference

in atomic hydrogen

J. P. Bouchaud and C. Lhuillier J. Physique 46 (1985) 1335-1344

One should notice that the collision integrals W given in figure 2 and table I differ from those defined and used in the text and appendix II by

factor

In figure 4 the quantity drawn is in fact n/k when k is the characteristic wavevector of the diffusion problem.

There is

factor 2 7r between the nL quantity defined in (22) and that drawn in figure 4.

Structural study of the charge density wave phase transition of the blue bronze :

K0.3MoO3

J.-P. Pouget, C. Noguera, A. H. Moudden and R. Moret J. Physique 46 (1985) 1731-1742.

1. The X-ray diffuse scattering intensity reported in section 3. 2 (see for example that shown in figure 5) has been

measured

the extra scattering above the background. Thus it cannot be accounted for by the equation :

which gives

absolute value of the diffuse intensity, without reference to the background With

background

contribution of kT In 2 co’, corresponding to the response of the unstable lattice mode in the absence of its coupling

with the electron gas, the measured diffuse intensity is actually given by :

where Y(q) is proportional to the CDW response function :

Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphys:01986004701014500

Longitudinal electronic and nuclear spin ^difference

J. P. Bouchaud and C. Lhuillier J. Physique ⁴⁶ (1985) ^1335-1344

One should notice that the collision integrals ^W given ⁱⁿ figure ² ^{and table} ^I differ from those defined and used in the text and appendix ^II by

^factor

In figure ⁴ ^the quantity drawn is in fact n/k when k is the characteristic wavevector of the diffusion problem.

factor 2 7r between the nL quantity defined in (22) and that drawn in figure ^4.

Structural study ^{of the} charge density ^wave phase transition of the blue bronze :

J.-P. Pouget, ^C. Noguera, ^{A. H.} Moudden and R. Moret J. Physique ⁴⁶ (1985) ^1731-1742.

1. The X-ray ^diffuse scattering intensity reported in section 3. 2 (see ^for example that shown in figure 5) ^{has been}

the extra scattering ^{above the} background. ^{Thus it} ^cannot ^be accounted for by ^the equation :

absolute value of the diffuse intensity, ^without ^reference ^to ^the background ^With

contribution of kT In 2 co’, corresponding ^to the response of the unstable lattice mode in the absence of its coupling

with the electron _gas, the measured diffuse intensity ^is actually given by :

where Y(q) ^is proportional ^to ^{the CDW} response function :