Rare Earths

256 Pages·1973·3.85 MB·English

by  R. A. Pennenvan, R. R. Ryan, A. Rosenzweig (auth.)

Contents
Structural Systematics in Actinide Fluoride Complexes. R .A .
Penneman R. R, Ryan, and A. Rosenzweig . . . . . . . . . . . . . . . . . . .
Spectra and Energy Transfer of Rare Earths in Inorganic Glasses.
Renata Reisfeld . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 58
The Crystal Chemistry of the Rare-Earth Silicates. J. Felsche . ..
The Inner Mechanism of Rare Earths Elucidated by Photo-Electron
Spectra. C. K. Jorgensen . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 199
Structural Systematics in Actinide Fluoride Complexes *
R. A. P e n n e m a n and R. R. Ryan
University of California, Los Alamos Scientific Laboratory
Los Alamos, New Mexico 87544/USA
A. R o s e n z w e i g
Department of Geology, University of New Mexico
Albuquerque, New Mexico 87106/USA
Table of Contents
1. Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1
1.1. Trends in Actinide Size and Valence . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3
1.2. Coordination Number and Polyhedra . . . . . . . . . . . . . . . . . . . . . . . . . . . . ' 4
1.3. Depolymerization by Fluoride; Variable Valence in Fluoride
Compounds . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 7
2. Structural Characteristics of Actinide Fluoride Complexes . . . . . . . . . . . . . . 8
2.1. Six Coordination . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8
2.2. Seven Coordination . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 12
2.3. Eight Coordination . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 15
2.4. Nine Coordination . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 28
2.5. List of Observed Stoichiometries by Element and Structure Type. 43
3. Optical Characteristics . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 43
3.1. Molar Refractivity . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 43
4. References . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 48
1. Introduction
Du r i n g t h e las t t w e n t y yea r s of ac t i ve i nves t i ga t i on , a large n u m b e r of
c rys ta l s t r uc t u r e s h a v e b e e n d e t e r m i n e d for c o m p o u n d s of t h e ac t in ides
w i t h f luorine. I t is t h e pu r po se of th is p a p e r to s u r v e y t h e s t r u c t u r a l
cha rac te r i s t i c s d i s p l a y e d b y these c o m p o u n d s . A m o n g the d - t r a n s i t i o n
e lements , t h e n u m b e r of d -e lec t rons has a s igni f icant effect on bond ing ,
a l t h o u g h th is effect is m i n i m u m in t he i r f luoro c o m p l e x e s (7). E v i d e n c e
of f -o rb i t a l p a r t i c i p a t i o n in ac t in ide f luor ide b o n d i n g has been s o u g h t (2) ;
however , th is s u r v e y will show t h a t t h e 5f -e lec t rons h a v e l i t t l e d i r ec t iona l
b o n d i n g effects in d e t e r m i n i n g ac t in ide - f luor ide c o m p l e x s t ruc tu res .
* This work was performed under the auspices of the U.S. Atomic Energy Com-
mission.
R. A. Penneman, R. R. Ryan and A. Rosenzweig
Actinide cations appear to behave in a largely ionic manner ; radius and
charge play a predominant role in the determination of structure and
coordination types (3).
The actinides (5f elements, Z = 90--103) offer to inorganic and struc-
tural chemists a unique oppor tuni ty for s tudy, since these elements
display a multiplici ty of valences (Fig. 1), as well as fixed valences for
+ 2 +3 + 4 @5 + 6 + 7
Ac X
Th X
Pa X X
U X X X X
Np X X X X ©
Pu X X X X ©
Am (X) X X ® ®
Cm X ®
Bk X ®
cf (x) x ®
Es (x) x
Fm X
Md X X
No X X
Lr X
@ Circles indicate valence achieved with oxygen
• Oxygen and fluorine
(X) Valence rare
Fig. 1. Actinide valences
upwards of a dozen consecutive elements. This latter aspect they share
with the lanthanide (4f) series, which, however, has a more monotonous
chemistry, being predominant ly tr ivalent with bu t few divalent and
te t ravalent species. The higher valence states of the actinides seem to be
achieved only in compounds with the highly electronegative ligands
oxygen and fluorine. The highest valence (+7) occurs with oxygen (d, 5,
6); for americium the + 5 and + 6 valences occur only in compounds
containing oxygen or bo th oxygen and fluorine (7, 8, 9) (Fig, 1). I t is
Structural Systematics in Actinide Fluoride Complexes
further noted that, excepting obvious chemical restrictions, the highest
oxidation states occur early in the series, while the stability of lower
valence states predominates in the last half of the series with the divalent
state occuring as early as californium (96). However, there is evidence
for Am(II) at low temperature in a CaF2 matrix (70) and recent work at
Oak Ridge and Los Alamos has established anhydrous divalent ameri-
cium halides (70a).
1.1. Trends in Actinide Size and Valence
Cation sizes have reached a maximum with the actinide ions and high
coordination numbers are demanded. The first actinide of a particular
charge is the largest elemental cation of that charge (thorium, for ex-
ample, is the largest M 4+ ion). Cell dimensions for oxides containing the
M 4+ actinides are known for nine successive elements (Th 4÷ through
Cf 4+) (77, 72); for M 3+ the data now extend through Es203 (13). Within
the 5f series, ionic sizes become demonstrably smaller with increasing
atomic number for the tri- and tetravalent ions. A similar pattern is
shown by the M 5+ species, with Pa 5+ being the largest (74), followed by
U 5÷, etc. (75). Pentavalent bismuth is the largest of the Group V, non-
transition elements in this oxidation state, but it is still smaller than U 5+
(NaBiF6 is isostructural with rhombohedral (76) NaUF6, but of smaller
cell dimensions (77)). When we compare the lanthanide (4f) and actinide
(5f) series with respect to relative trivalent ion sizes, we find that those
of the latter series are larger and that, for example, trivalent californium
is the size of the trivalent lanthanide, europium (77), three elements be-
fore the 4f counterpart of californium. Although there are fewer data on
tetravalent lanthanides to compare, we find the same general size dis-
placement of the tetravalent 5f ions with respect to their 4f analogs,
Ce 4+ being smaller than U 4+ and Tb 4+ than Cf 4+.
In Fig. 2, the actinide element (in its various valences) is written
beneath each last row element if it displays that group valence. Uranium,
for example, is shown in the last row in its customary position between
protactinium and neptunium; additionally, it is written beneath actin-
ium to indicate that uranium has a tri-positive state and under thorium,
since uranium has a tetra-positive state, etc. This has the effect of pivot~
ing the bottom row of the periodic table at each actinide, bringing those
elements to its right beneath it. The pivot element displays the maximum
ion size for that particular valence. General group chemical similarity is
displayed within a column. However, the reduction in ion size as the
atomic number increases may cause differences such as change in coor-
dination, which results in the appearance of analogous compounds which
are isostoichiometric but not isostructural.
R.A. Penneman, R. R. Ryan and A. Rosenzweig
U" HI IV V VI ~i v A
I Sr Y Z r Nb Mo Tc Sb ~ USUAL
ION SIZE
I Ba La-Lu Ce-HF Ta W l~e Bi I PERIODIC
INCREASES i Ra Ac Th Pa U
ITp TABLE
T ACTINIDE VALENCES
(Th) Pa Pa
NaBiF6 l
U U U U
<NaUF~l
Np Np Np Np Nn
Pu IAt IAt IAt Pu
Am Am Am Am Am
ION SIZE
Cm Cm
INCREASES
Bk Bk
Cf Cf
Es
Fra
Md Md
No No
Lr ION SIZE INCREASES
Fig. 2. Modi f ied pe r iod ic t ab l e , s h o w i n g v a l e n c e l o c a t i o n of a c t i n i de s a n d size t r e n d s
1"21 I I
l.I
De I ACTINIDES +31
o< 9 -
rv / t7 COOR'D. \ ~ -----_...~a 8-
s COOR'D " \
_ o.B 7 -
I ACT'NtDES+41
02 I,'%__ COORDINATION
NUMBER
6 COOR'D 6
0.6 l
o.s I I
o+.,+, , io
+6 f ELECTRONS
Fig . 3. I o n i c r a d i i o f s o m e ac f in ides a n d l a n t h a n i d e s ill v a r i o u s v a l e n c e s
1.2. Coordinat ion N u m b e r and Po lyhed ra
In Fig. 3 are shown some ionic radi i for M 3+, M 4+, and M 5+ ox ida t ion
s tates . Ionic radi i vary , depending on choice of counter ion radius, model
compounds, coordina t ion number , etc. F o r a recent review see Shannon
Structural Systematics in Actinide Fluoride Complexes
and Prewitt (18). Most of the radii used in Fig. 3 are those of Zacharia-
sen (79) and of Peterson and Cunningham (17), who compared similar
lanthanide and actinide compounds. Ions of both series are obviously
large and of a size sufficient to preclude lower than six coordination with
F - and to make six coordination a rarity. In the review by Muetterties
and Wright it was noted that tile actinide and lanthanide fluorides favor
high coordination numbers (20). Excellent illustrations of high coordi-
nation number polyhedra are found in their paper. In his book, D. Brown
devotes a chapter to fluorides and oxyfluorides of the lanthanides and
actinides (20 a).
Table 1
Octahedron 6 0.55 X
Capped octahedron 7 0.79
Antiprism 8 0.86
Dodecahedron 8 0.89
Cube 8 0.97
Tricapped trigonal prism 9 0.97
The coordination polyhedra, coordination number, and maximum size
of coordinated metal ion which will just allow F - -F hard sphere contacts
are given in Table 1. Coordination numbers of 6--9 are thus expected for
actinide fluorides, (see Fig. 3) with 6 being attained only for valences
greater than 4 +. Eight coordination spans tile largest range of radius
ratios, and extends to the nine-coordination radius ratio. Coordination of
the majori ty of actinide ions to fluoride ion (1.33 A) yields radius ratios
within this range. We expect highest coordination numbers to be ob-
served at the actinide element where a given charge type first occurs,
since it is the largest ion of its type. As the size diminishes with atomic
number, we can anticipate changes to occur such as diminution of coor-
dination number, and recurrence of structures previously observed for
the smaller d-transition elements. For example, K2UF7 and K2TaF7
are isostructural with coordination number 7 for tile pentavalent ele-
ment, but K2PaF7 has a different structure and coordination number of
9 for protactinium (V) (ld).
In 1948 Zachariasen (27), studying a number of alkali actinide fluor-
ides, noted that the cell volumes of these compounds could be at tr ibuted
to the volume of the fluoride ions and the larger alkali ions alone, with
the actinide ions occupying interstices between the anions. In his exam-
ples he assigns a volume of 18 A s for F- , 7 A a for Na+, and 21 flta for K +,
etc. This relationship is borne out in many structures of related com-
R. A. Penneman, R. R. Ryan and A. Rosenzweig
pounds which have since been determined. The tri- and tetravalent
actinide ions are quite large (similar to Na+), and the fluorine volume
deduced from measured cell volumes includes a contribution from the
actinide. The difference in actinide size and coordination would produce
variation in effective F - volume, but this variation will be small because
of the generally large coordination number of the actinide. Thus, known
stoichiometry leads to a useful estimation of volume/formula wt, which
is essentially independent of structure, as are other functions of volume,
such as the Lorentz-Lorenz molar refractivity (22).
These observations lead one to suspect that the fluoride ions and larger
alkali ions in these compounds are arranged in an approximation of a
close packed array. These suspicions are easily confirmed by an inspection
of the available structural data. The details of the close packed array are
strongly influenced by the alkali ion size. The smallest can be accommo-
dated in the interstices of a fluoride anion array, but as the cation size
increases the array will be progressively distorted, and ultimately the
alkali may become a part of the close packing scheme. These two ex-
tremes are exemplified by the following: In LiUF6 (LiSbF6 type (23)
the alkali and actinide are relatively small and occupy octahedral sites
in an array of fluorides which approximates a hexagonal close-packed
array. In the compounds KUF6 and RbUF6 the alkali ions are ten coor-
dinate and the actinide eight-coordinate (2d), but the model for the pack-
ing is difficult to describe. In CsUF6 the U 5+ again occupies an octa-
tledral site but the large Cs + is twelve-coordinated; the cesium and fluor-
ine, in this case, make up a distorted cubic close-packed array (75). In
Na3PaFs (25) the fluorines are less densely packed (cube corners) and
both Na + and Pa 5+, though much smaller than fluorine, become part of
the distorted cubic close-packed array. Further distortions are caused by
such phenomena as hydrogen bonding and cation-cation repulsions. A
striking example of the first of these is seen in the pair of compounds
Rb2UF6 and (
Structural Systematics in Actinide Fluoride CompIexes
1.3. Depolymerization by Fluoride; Variable Valence in Fluoride
Compounds
To achieve high coordination number, the binary fluorides MFx of the
actinides are polymeric, with fluorines being shared between two or
more actinides (an obvious exception to this is presented by the low-
boiling MF6 fluorides). In the usual case, the MFx unit in the lattice is
part of a chain or of a three dimensional polymer. For example, eight
coordinated UF4 has all fluorides shared. However, it can be depolymer-
ized by addition of alkali fluoride, successively passing through a series
. . . . a -
of complexes terminating at the discrete anionic species UFs . In chain
structures, the distance between nearest neighbor actinides is about
4 •; in structures having isolated anions they are much farther apart.
In the case of KhThF9 further "dilution" occurs and the structure con-
tains ThFs4 - ions as well as F - ions which are "free" in the sense of not
being bound to thorium. There are cases in which "dilution" by free
fluoride causes no further depolymerization: (NH4) aThF7 and
(
R.A. Penneman, R. R. Ryan and A. Rosenzweig
bers. Change in valence of the kernel actinide is frequently accompanied
by a change in coordination number. However, this may leave the heavy
atom positions essentially unchanged. This is illustrated by the structures
of Na2UFs and Na3UFT, which are derived from NasUFs as follows:
(--Na)
(--F) ~ Na2UFs
Na3UF8
NaaUF7
Thus, Na~UFs has sodium ion vacancies and NaaUF7 has fluoride
ion vacancies. An additional example is provided by a series of uranium
compounds in which the parent fcc cell of ~-~9.2 ~ can accommodate
3 KF • UF3, 3 KF • UF4, or 3 K F . UFs, and whose powder patterns
are essentially indistinguishable (28). Additional substances with similar
unit cells are listed by Wyckoff (29).
2. S t ruc tu ra l Character is t ics of A c t i n i d e F l u o r i d e Complexes
2.1. Six-coordinated Actinide-fluoride Complexes
The structural chemistry of six-coordinated fluoro complexes of the
d-transition elements is the subject of an entire review paper by Babel (1).
In contrast, six coordination is rare in actinide fluoro-complexes. The
relatively large sizes of the actinide ions (Fig. 3) suggest that low coor-
dination numbers should be found only in the fluoride complexes of the
higher oxidation states. The radius ratio, r+/r -, predicted for the lower
limit of stability of octahedral coordination is V~ - 1, which corresponds
to a positive ion radius of 0.55 • in coordination with fluoride (1.38 A).
Of the very few known structure types displaying six-coordinated
actinides, only two, UF6 and CsUF6, have been determined with suf-
ficient accuracy to give trustworthy values for the effective ionic radii
of the actinide ions. In UF6 and CsUF6 the uranium ions (U 6+ and U 5+)
have radius ratios with fluorine well above the lower limit of stability
for octahedral coordination but still lower than the lower limit predicted
for the 8-coordinated square antiprism (0.645) or the 7-coordinated
capped octahedron (0.592). However, both U 6+ and U 5+ are sufficiently
larger than 0.55 A so that F- -F distances in the octahedron cannot all
be van der Waals' contact distances, and thus, the MF6 octahedra are
susceptible to distortion.
8
Structural Systematics in Actinide Fluoride Complexes
Isolated octahedral groups are found in orthorhombic UF6 (,30).
Within the accuracy of the single crystal X-ray experiment the coor-
dination was not demonstrated to be significantly distorted from that of
a regular octahedron. The average U--F distance of 2.05 • gives an
effective U 6+ radius of 0.72 A.
There are several examples of isolated MF~ ions which are slightly
distorted from ideal octahedral geometry (Table 2). In the rhombo-
hedral CsUF6 (15), (see Fig. 4) Us+ has six fluorine neighbors at the
corners of an octahedron which is slightly elongated (stated as flattened
in Ref. (15)) along the three-fold axis (symmetry D3d). The angle be-
tween the trigonaI axis of the UF~ group and a U--F bond is 53 ° 23',
smaller than the value 54 ° 44' for a regular octahedron. The U--F
distance is 2.057 A, giving an effective U 5+ radius of 0.73 •. The cesium
ion in CsUF6 is twelve-coordinated, having six fluorines at 3.10 ,~ and
six more F neighbors at a slightly longer distance (3.17 A) (75). Cesium is
located on the trigonal axis and separates two UF~ polyhedra. The com-
pounds CsNpFa (31) and CsPuF6 (32) are isostructural with CsUF6.
These structures are of the KOsF6 (33) type, which was determined only
from powder data.
6 COORDINATION
TRIGONAL PRISM OCTAHEDRON
¢suFe
L~UF~
UNKNOWN
NaUF6
FOR
ACTINIDES
Fig. 4. Polyhedra for six-coordinated actinides
The X-ray powder patterns of LiUF6 (34) and of a-NaUF6 (16)
indicate that they are both isostructural with rhombohedral (R3)
9