In table V: The units for the zeroth, first, and second spectral moments should be
erg cm
6, erg cm
6/s, and erg cm
6/s
2, respectively.
Regarding Eq. (A2): The second row should end with
dE and
the second × (times) symbol, on the third row, should be a + (plus).
The triangular line profile in Eq. (7) is non-zero only when
ν
k'kJ'J-w < ν < ν
k'kJ'J+w.
The triangular line profile in Eq. (16) is non-zero only when
ν
n'nJ'J-ω < ν < ν
n'nJ'J+ω.
The last sentence of section 5.1.3 should read:
These coefficients include a factor 1/√3, which would otherwise have appeared as 1/3 in Eq. (16),
and they account for the angular momentum selection rules
- total angular momentum: J' = J; J±1
- j and j' are both even or both odd
- parity must change, implying that l changes from odd to even or vice versa.
On the left hand side in Eq. (5) the probability should have superscript
i → all f.
It is thus distinct from the two-state probability
i → f in Eq. (6).
Fig. 1, the upper inset, which concerns dipole moments: The vertical axis should display atomic units of dipole moment.
The numbers in the published figure (−30 and −60) should be divided by 27.211.
The numbers in the data file, which is provided as supplementary material, are correct.
In table IV the value of Ω' should equal 1 on the first and second row.
The value of Ω should equal 1 on the third and fourth row.
J. Chem. Phys. 130, 164314 (2009): (typos)
- There are three equations without equation numbers between Eqs. (B1) and (B2).
In the middle one of those (the one with DID) the right hand side should be multiplied
by a factor sqrt(2/3).
- In the middle relation in Eq. (B2) (the one with DID) the factor sqrt(3/2) should
go out.
The summation index
V' in equation (14) should be a lower case
v' (Greek nu').
On the other hand, the lower case
v inside the summation
should be a captital
V.
J. Chem. Phys. 115, 5427 (2001): (comment on parameter values)
The a, b, and d parameter values in table III are given with too few
significant digits to correctly reproduce the collision-induced background
absorption, especially in the fundamental band. Better values are given
below.
| a | b |
d |
R0(0) | -0.208977[-6] |
0.876095[-8]
| -0.306704[-10] |
R0(1) | 0.628021[-6] |
-0.220323[-8]
| 0.611017[-11] |
P1(1) | 0.419582[-3] |
-0.241736[-6]
| 0.348191[-10] |
R1(0) | -0.331911[-3] |
0.185684[-6]
| -0.258495[-10] |
R1(1) | 0.275607[-3] |
-0.140382[-6]
| 0.179002[-10] |
J. Chem. Phys. 113, 3641 (2000): (typos)
- On the right hand side of equation (4) the factor 1/(n!)
should go out.
- Third paragraph, second sentence on page 3643; replace with:
The signs of the radial wave functions
have been fixed so that they 'start' positive, going from r=0.
- On the right hand side of equation (8) the minus sign should be replaced
by a plus sign.
- On the right hand side of equation (22) the factor r should go
out.
- The right hand side of equation (29) should be multiplied by a factor
sqrt(3)/(4 pi)