Density functional molecular dynamical simulations have been performed on
Ga$_{17}$ and Ga$_{13}$ clusters to understand the recently observed
higher-than-bulk melting temperatures in small gallium clusters [Breaux {\em et
al.}, Phys. Rev. Lett. {\bf 91}, 215508 (2003)]. The specific-heat curve,
calculated with the multiple-histogram technique, shows the melting temperature
to be well above the bulk melting point of 303 K, viz. around 650 K and 1400 K
for Ga$_{17}$ and Ga$_{13}$, respectively. The higher-than-bulk melting
temperatures are attributed mainly to the covalent bonding in these clusters,
in contrast with the covalent-metallic bonding in the bulk.Comment: 4 pages, including 6 figures. accepted for publication in Phys. Rev.
  Let

D. G. Kanhere

D. G. Kanhere

D. J. Wales

Kavita Joshi

P. Pawlow

R. S. Berry

S. A. Blundell

S. Chacko

V. Heine

V. Heine

English

arXiv

Density functional molecular dynamical simulations have been performed on Ga17 and Ga13 clusters to understand the recently observed higher-than-bulk melting temperatures in small gallium clusters [G.A. Breaux et al., Phys. Rev. Lett. 91, 215508 (2003)]. The specific-heat curve, calculated with the multiple-histogram technique, shows the melting temperature to be well above the bulk melting point of 303 K, viz., around 650 and 1400 K for Ga17 and Ga13, respectively. The higher-than-bulk melting temperatures are attributed mainly to the covalent bonding in these clusters, in contrast with the covalent-metallic bonding in the bulk

Chacko, S.

Joshi, Kavita

Kanhere, D. G.

Blundell, S. A.

Indian Academy of Sciences

Why do gallium clusters have a higher melting point than the bulk?

Publications of the IAS Fellows

P H Y S I C A L R E V I E W L E T T E R S week ending2 APRIL 2004VOLUME 92, NUMBER 13Why Do Gallium Clusters Have a Higher Melting Point than the Bulk?
S. Chacko, Kavita Joshi, and D. G. Kanhere
Department of Physics and Center for Modelling and Simulation, University of Pune, Pune - 411 007, India
S. A. Blundell
De´partement de Recherche Fondamentale sur la Matie`re Condense´e, CEA-Grenoble/DSM,
17 rue des Martyrs, F-38054 Grenoble Cedex 9, France
(Received 11 December 2003; published 2 April 2004)135506-1Density functional molecular dynamical simulations have been performed on Ga17 and Ga13 clusters
to understand the recently observed higher-than-bulk melting temperatures in small gallium clusters
[G. A. Breaux et al., Phys. Rev. Lett. 91, 215508 (2003)]. The specific-heat curve, calculated with the
multiple-histogram technique, shows the melting temperature to be well above the bulk melting point
of 303 K, viz., around 650 and 1400 K for Ga17 and Ga13, respectively. The higher-than-bulk melting
temperatures are attributed mainly to the covalent bonding in these clusters, in contrast with the
covalent-metallic bonding in the bulk.
DOI: 10.1103/PhysRevLett.92.135506 PACS numbers: 61.46.+w, 36.40.Cg, 36.40.Eitemperature behavior of clusters [6]. For example, almost
all simulations carried out to explain the thermodynamic
Isokinetic Born-Oppenheimer MD simulations have
been carried out using ultrasoft pseudopotentials withinProbing finite-temperature properties of clusters is a
challenging task, both experimentally and theoretically.
During the last few years a number of intriguing aspects
of the melting properties of these finite-sized systems
have been observed, such as a negative microcanonical
specific-heat [1] and substantially higher melting tem-
peratures than the bulk systems [2]. In a series of experi-
ments on free sodium clusters (with sizes ranging from 55
to 357 atoms), Haberland and co-workers [3] observed a
substantial lowering (by about 30%) of melting tempera-
tures compared to bulk sodium, with rather large size-
dependent fluctuations in the melting temperatures. This
lowering is in qualitative agreement with old thermody-
namic arguments [4] that a small particle should melt at a
lower temperature than the bulk because of the effect of
the surface. However, Shvartsburg and Jarrold [2] showed
recently that small tin clusters (with sizes between 10 and
30 atoms) do not melt at least 50 K above the bulk melting
temperature. Surprisingly, a very recent measurement on
small gallium clusters by Breaux et al. [5] presented
another example of a higher-than-bulk melting tempera-
ture. Their measurements indicated that Ga17 does not
melt up to about 700 K, while Ga39 and Ga40 have
melting temperatures of about 550 K, all well above the
bulk melting point [Tmbulk  303 K]. While it might
have been thought that tin was an exceptional case, these
new measurements suggest that elevated melting tem-
peratures could perhaps be a more widespread phenome-
non. These authors also investigated the fragmentation
pattern but were unable to find the existence of any
particular stable building block, and they did not offer
any explanation for the high melting temperatures.
Traditionally, classical molecular dynamics (MD)
simulations have been used to understand the finite-0031-9007=04=92(13)=135506(4)$22.50data of sodium clusters are based on classical MD em-
ploying a variety of parametrized interatomic potentials
[7]. However, these attempts have fallen short of repro-
ducing the crucial characteristics observed experimen-
tally, such as the precise sizes at which maxima in the
melting temperatures occur. Quite clearly, for reproduc-
ing the experimental results a more realistic treatment of
interacting electrons is desirable. Recently, we have suc-
cessfully demonstrated the power of density functional
molecular dynamics (DFMD) by providing a detailed
explanation of the experimentally observed phenomena
of higher-than-bulk melting temperatures for tin clusters
[8]. In particular, we have shown that the covalent bond-
ing along with the existence of a highly stable tricapped
trigonal prism (TTP) subunit is responsible for the higher
melting temperature. For gallium clusters also, an
ab initio treatment is quite crucial for simulating the
finite-temperature behavior, especially since there is a
possibility of a change in the nature of the bonding.
In this Letter, we provide an explanation and insight
into the phenomenon of the higher-than-bulk melting
temperature recently observed in small gallium clusters
[5]. To this end we have carried out ab initio density
functional simulations over a wide range of temperatures
for the neutral clusters Ga17 and Ga13. We present the cal-
culated specific heat obtained via a multiple-histogram
(MH) analysis [9]. We also present a detailed analysis of
bonding in these clusters and contrast it with that of bulk.
In an earlier density functional calculation by Jones, the
bonds in small gallium clusters have been found to be
shorter than those between the lighter atoms in the same
main group, i.e., Al [10]. As we shall see, these clusters
indeed melt at a temperature substantially higher than
Tmbulk, mainly due to the formation of covalent bonds. 2004 The American Physical Society 135506-1
P H Y S I C A L R E V I E W L E T T E R S week ending2 APRIL 2004VOLUME 92, NUMBER 13the local density approximation, as implemented in the
VASP package [11]. For Ga17, the MD calculations were
carried out for 23 temperatures, each of duration 75 ps, in
the range of 150  T  1100 K, which results in a total
simulation time of 1.65 ns. The resulting trajectory data
have been used to compute the ionic specific heat by
employing the MH method [9,12]. For all the calcula-
tions, we have used only sp electrons (4s2 and 4p1) as
valence electrons, taking 3d as a part of the ionic core
(represented by an ultrasoft pseudopotential). We have
verified that the d electrons do not significantly affect
the finite-temperature behavior and equilibrium geome-
tries by recalculating the equilibrium structures, and
performing three runs at finite temperature around the
melting region, with the d electrons treated explicitly as
valence electrons.
We begin our discussion by noting some interesting
features of the electronic structure of bulk Ga, which
has been investigated by Gong et al. [13]. The -Ga lat-
tice, which is stable at ambient pressure, can be viewed as
base-centered orthorhombic with eight atoms in the unit
cell. The peculiarity of this structure is that each atom
has only one nearest neighbor connected by a short bond
at a distance of 2:44 A(see Fig. 1). The six other neighbors
are at distances of 2.71 and 2:79 A, in two sets of three.
These six atoms lie on strongly buckled parallel planes
connected by the short bonds, as shown in Fig. 1. Elec-
tronic structure calculations by Gong et al. [13] reveal
this short bond to be covalent in nature. The density of
states shows a pseudogap, which has been related to this
covalent bond [14], and the weak bonding in the buckled
planes leads to an observed metallic behavior. Thus, two
kinds of bonds coexist in bulk Ga: one a molecular bond
between the nearest neighbors and the other a metallic
bond within the buckled planes.
Now we present and discuss some relevant features
observed in the equilibrium structures of Ga17. We have
relaxed many structures, randomly chosen from high-
temperature DFMD runs. In this way, we have found
more than 20 different equilibrium structures spanningFIG. 1. A part of the bulk structure of -Ga (not a unit cell).
It shows two buckled planes. The dark line joining the black
atoms corresponds to the interplanar covalent bond discussed
in the text.
135506-2an energy range of about 0.83 eV with respect to the
ground-state energy. In Fig. 2, we show some low-lying
structures relevant to the present discussion. A common
feature observed in all these geometries, except one
[Fig. 2(d)], is the presence of a trapped atom, that is, a
single atom contained within a cage formed by the re-
maining atoms. The lowest-energy structure that we have
found [Fig. 2(a)] is a highly asymmetric structure, which
can be thought of as formed out of a decahedron with
serious distortions and asymmetric capping. Interest-
ingly, this structure can also be viewed as composed of
two near planar rings, as discussed further below.
We have also analyzed the nature of bonding by em-
ploying the electron localization function (ELF) [15],
which is defined such that values approaching unity in-
dicate a strong localization of the valence electrons and
covalent bonding. The isosurface of the ELF for the
neutral Ga17 and charged Ga17 are shown in Figs. 3(a)
and 3(b), respectively. A striking feature seen in these
figures is the existence of strong localized bonds giving
rise to two ringlike structures. Further, these rings are
also bonded to each other via the atoms at the edge of each
ring and with the trapped atom at the center. The exis-
tence of an isosurface of the ELF with such a high value
clearly indicates the covalent nature of the bonding. This
is also substantiated by examination of the corresponding
charge-density isosurface (not shown). Calculations of
the ELF for the excited isomers in Fig. 2 and for other
small Ga clusters show similar features. Generally, most
atoms have two covalent bonds in a roughly linear ar-
rangement, with a tendency to link neighbors together
into rings or ring fragments; extra covalent bonds on
some atoms then join these structures together. The bond-
ing here is thus seen to be in sharp contrast to the one
observed in the bulk -Ga, where, as discussed earlier,
only a single strong interlayer bond between two GaFIG. 2. The ground-state geometry and some of the the low-
energy structures of Ga17. The structures are arranged in
increasing order of the energy. (a) represents the lowest-energy
structure and (d) represents the highest-energy structure
studied. Energy differences E are in eV.
135506-2
1.4
v
/C
0)
P H Y S I C A L R E V I E W L E T T E R S week ending2 APRIL 2004VOLUME 92, NUMBER 13atoms exists (see Fig. 1). An analysis of the bond lengths
reveals that each atom in the cluster has at least two near-
est neighbors at a distance of 2:5 A or less. Indeed, it is
this difference in bonding that is primarily responsible
for the higher melting temperature of the small clusters.
An examination of the molecular orbitals and the ei-
genvalue spectrum (not shown) brings out some notable
features. The eigenvalue spectrum is divided into two
groups, which are separated by about 1.18 eV. The lower
15 states forming the first group are the bonding states
formed out of atomic 4s orbitals. Almost all the upper
states are formed out of pure atomic p orbitals and show
no sp hybridization. The only exception to this is the
bonding between the trapped atom and its three nearest
neighbors, where a weak sp2 hybridization is observed.
This picture is also confirmed by a site-projected spheri-
cal harmonics analysis of the orbitals, which does not
show any significant mixing of s and p character in these
states. All the bonds seen are of predominantly 
 type,
formed out of atomic s and p orbitals. The lack of sp
hybridization explains the tendency to form covalent
bonds at approximately 180 or 90 angles, as observed
in Fig. 3.
The calculated specific-heat curve for Ga17 is shown in
Fig. 4. A clear peak is observed in the specific heat with a
maximum around 650 K, well above the bulk melting
point of 303 K. Following the discussion in Ref. [8], we
expect the statistical uncertainty in our peak position to
be up to 15%. Now, a novel multicollision induced disso-
ciation scheme has recently been used to measure the
caloric curve of small, charged Ga clusters [5]. For
Ga17

, no evidence was found for melting (in the sense of
a peak in the specific heat) over a temperature range 90–
720 K. Our simulations are consistent with this finding.
Note that there is likely to be some shift of the melting
temperature between the neutral and charged cluster.
While the thermodynamic simulation has been carried
out for neutral Ga17, calculations of the ELF in Ga17
reveal a similar network of covalent bonds [see Fig. 3(b)].
The ground-state geometry changes to a more symmetric
form (which is a low-lying isomer for Ga17), and the
HOMO-LUMO (highest occupied molecular orbital–
lowest unoccupied molecular orbital) gap increasesFIG. 3. The isosurface of ELF for (a) Ga17 at the value 0.68
and (b) Ga17 at the value 0.65.
135506-3from 0.76 eV for the neutral to 1.07 eV. The low-lying
isomers span an energy range of order 0.8 eV for both Ga17
and Ga17. Therefore, we expect Ga17 to have similar
melting properties to Ga17. The larger HOMO-LUMO
gap for Ga17 may imply that it has a slightly higher
melting temperature.
Our specific-heat curve shows no premelting features
in the temperature range studied, and that the peak is
quite broad, as expected for the finite-sized systems. A
detailed examination of the ionic motion at different
temperatures sheds more light on the nature of melting.
Around 225 K, we observe the occurrence of the first
excited state [Fig. 2(b)]. As the temperature rises further,
the system visits a variety of isomers all of which contain
a trapped atom. It is only above 550 K that the isomer
shown in Fig. 2(d) is observed. Evidently, the peak in the
specific heat is associated with the diffusion of the
trapped atom out of the enclosing structure. Interest-
ingly, in the trajectories at all temperatures below
600 K, the trapped atom is seen to bond itself to atoms
in both rings. This confers stability on the caged struc-
ture. We have also carried out the analysis of the melting
properties via traditional parameters such as the root-
mean-square bond-length fluctuations and the mean
square atomic displacements (not shown). Their behavior
is consistent with the above observations.
To summarize, our ab initio MD simulations have
shown that the elevated melting temperature of Ga17 is
due mainly to the formation of covalent bonds. The
stability of the cluster is further enhanced by the role of
the caged atom. These observations should have implica-
tions for the melting characteristics of clusters of smaller
sizes, such as Ga13. The ground-state geometry of Ga13 is
decahedral, a more compact structure having a greater
average number of covalent bonds per atom than Ga17.
Further, our bonding analysis shows that the bonding is
strongly covalent, similar to Ga17. We therefore expect
this cluster to melt at a higher temperature than Ga17. To1.08
1.16
1.24
1.32
300 450 600 750 900 1050
Ca
no
ni
ca
l S
pe
ci
fic
 H
ea
t (
C
Temperature (K)
FIG. 4. Normalized canonical specific heat of Ga17 cluster.
C0  3N  9=2kB is the zero temperature classical limit of
the rotational plus vibrational canonical specific heat.
135506-3
FIG. 6. The isosurface of ELF for Ga40 at the value 0.64.
1
1.2
1.4
1.6
1.8
400 700 1000 1300 1600
Ca
no
ni
ca
l S
pe
ci
fic
 H
ea
t (
C v
/C
0)
Temperature (K)
FIG. 5. Normalized canonical specific heat of Ga13 cluster.
P H Y S I C A L R E V I E W L E T T E R S week ending2 APRIL 2004VOLUME 92, NUMBER 13verify this conjecture, we have carried out extensive
DFMD simulations for 30 different temperatures in the
range 40  T  1750 K, with a total simulation time of
about 2.7 ns. The resulting specific heat is shown in Fig. 5.
Indeed, the peak is around 1400 K, a much higher value
than the peak position of Ga17 or the bulk melting point.
The detailed analysis will be published elsewhere.
Finally, we note that Ga39 and Ga40 have been
measured to have a broad maximum in the specific heat
around 550 K [5]. Unfortunately, the large sizes of these
clusters prevent us from making a complete thermody-
namic study at this stage. However, we have found and
analyzed some low-lying equilibrium structures of Ga40.
We believe that a mechanism similar to that in Ga17 is
operative in Ga39 and Ga40. In Fig. 6 we show an
isosurface of the ELF for the value of 0.64 for Ga40.
The ringlike structures of covalent bonds are once again
clearly evident. However, it may be noted that at this
value of the ELF no contours are seen between the inner
core atoms and the outer surface, and not all the atoms on
the surface are bonded. Therefore, it is not unreasonable
to expect this cluster to melt at a somewhat lower tem-
perature than Ga17, but still higher than that of the bulk.
In conclusion, we have carried out extensive density
functional thermodynamical simulations on Ga17 and
Ga13 with the aim of understanding the observed
higher-than-bulk melting temperatures. The analysis of
the specific-heat curve indicates the melting temperatures
(defined as the peak of the specific-heat curve) to be
around 650 and 1400 K for Ga17 and Ga13, respectively.
This result is consistent with the recent experimental
observations of Breaux et al. [5]. We find a significant
change in the nature of bonding between bulk Ga and
small Ga clusters. The strong covalent bonds in the small
clusters, along with the stabilizing role of the trapped
atom in Ga17, are responsible for the higher-than-bulk
melting temperatures. While the structural details for Sn
and Ga clusters are very different, the common feature135506-4between these two systems is thus seen to be the develop-
ment of strong covalent bonding in the small clusters.
One of us (S. C.) acknowledges financial support
from CSIR (New Delhi). It is a pleasure to acknowledge
C-DAC (Pune) for providing us with supercomputing
facilities.[1] M. Schmidt, R. Kusche, Th. Hippler, J. Donges,
W. Kronmu¨ller, B. von Issendorff, and H. Haberland,
Phys. Rev. Lett. 86, 1191 (2001).
[2] A. A. Shvartsburg and M. F. Jarrold, Phys. Rev. Lett. 85,
2530 (2000).
[3] M. Schmidt and H. Haberland, C. R. Physique 3, 327
(2002); M. Schmidt, R. Kusche, W. Kronmu¨ller,
B. von Issendorff, and H. Haberland, Nature (London)
393, 238 (1998).
[4] P. Pawlow, Z. Phys. Chem. (Leipzig) 65, 1 (1909);
Ph. Buffat and J.-P. Borel, Phys. Rev. A 13, 2287 (1976).
[5] G. A. Breaux, R. C. Benirschke, T. Sugai, B. S. Kinnear,
and M. F. Jarrold, Phys. Rev. Lett. 91, 215508 (2003).
[6] R. S. Berry, Int. J. Mod. Phys. B 6, 3695 (1992); D. J.
Wales, Mol. Phys. 78, 151 (1993).
[7] F. Calvo and F. Spiegelmann, J. Chem. Phys. 112, 2888
(2000); N. Ju and A. Bulgac, Phys. Rev. B 48, 2721
(1993).
[8] Kavita Joshi, D. G. Kanhere, and S. A. Blundell, Phys.
Rev. B 66, 155329 (2002); 67, 235413 (2003).
[9] A. M. Ferrenberg and R. H. Swendsen, Phys. Rev. Lett.
61, 2635 (1988); P. Labastie and R. L. Whetten, Phys.
Rev. Lett. 65, 1567 (1990).
[10] R. O. Jones, J. Chem. Phys. 99, 1194 (1993).
[11] Vienna ab initio simulation package, Technische
Universita¨t Wien, 1999; G. Kresse and J. Furthmu¨ller,
Phys. Rev. B 54, 11169 (1996).
[12] D. G. Kanhere, A. Vichare, and S. A. Blundell, Reviews in
Modern Quantum Chemistry, edited by K. D. Sen (World
Scientific, Singapore, 2001).
[13] X. G. Gong et al., Phys. Rev. B 43, 14 277 (1991).
[14] V. Heine, J. Phys. C 1, 222 (1968);V. Heine and D.Weaire,
Solid State Phys. 24, 249 (1970).
[15] B. Silvi and A. Savin, Nature (London) 371, 683 (1994).135506-4


Crossref

Why Do Gallium Clusters Have a Higher Melting Point than the Bulk?

P H Y S I C A L R E V I E W L E T T E R S week ending
2 APRIL 2004VOLUME 92, NUMBER 13Why Do Gallium Clusters Have a Higher Melting Point than the Bulk?
S. Chacko, Kavita Joshi, and D. G. Kanhere
Department of Physics and Center for Modelling and Simulation, University of Pune, Pune - 411 007, India
S. A. Blundell
Département de Recherche Fondamentale sur la Matière Condensée, CEA-Grenoble/DSM,
17 rue des Martyrs, F-38054 Grenoble Cedex 9, France
(Received 11 December 2003; published 2 April 2004)135506-1Density functional molecular dynamical simulations have been performed on Ga17 and Ga13 clusters
to understand the recently observed higher-than-bulk melting temperatures in small gallium clusters
[G. A. Breaux et al., Phys. Rev. Lett. 91, 215508 (2003)]. The specific-heat curve, calculated with the
multiple-histogram technique, shows the melting temperature to be well above the bulk melting point
of 303 K, viz., around 650 and 1400 K for Ga17 and Ga13, respectively. The higher-than-bulk melting
temperatures are attributed mainly to the covalent bonding in these clusters, in contrast with the
covalent-metallic bonding in the bulk.
DOI: 10.1103/PhysRevLett.92.135506 PACS numbers: 61.46.+w, 36.40.Cg, 36.40.Eitemperature behavior of clusters [6]. For example, almost
all simulations carried out to explain the thermodynamic
Isokinetic Born-Oppenheimer MD simulations have
been carried out using ultrasoft pseudopotentials withinProbing finite-temperature properties of clusters is a
challenging task, both experimentally and theoretically.
During the last few years a number of intriguing aspects
of the melting properties of these finite-sized systems
have been observed, such as a negative microcanonical
specific-heat [1] and substantially higher melting tem-
peratures than the bulk systems [2]. In a series of experi-
ments on free sodium clusters (with sizes ranging from 55
to 357 atoms), Haberland and co-workers [3] observed a
substantial lowering (by about 30%) of melting tempera-
tures compared to bulk sodium, with rather large size-
dependent fluctuations in the melting temperatures. This
lowering is in qualitative agreement with old thermody-
namic arguments [4] that a small particle should melt at a
lower temperature than the bulk because of the effect of
the surface. However, Shvartsburg and Jarrold [2] showed
recently that small tin clusters (with sizes between 10 and
30 atoms) do not melt at least 50 K above the bulk melting
temperature. Surprisingly, a very recent measurement on
small gallium clusters by Breaux et al. [5] presented
another example of a higher-than-bulk melting tempera-
ture. Their measurements indicated that Ga17
 does not
melt up to about 700 K, while Ga39
 and Ga40
 have
melting temperatures of about 550 K, all well above the
bulk melting point [Tmbulk  303 K]. While it might
have been thought that tin was an exceptional case, these
new measurements suggest that elevated melting tem-
peratures could perhaps be a more widespread phenome-
non. These authors also investigated the fragmentation
pattern but were unable to find the existence of any
particular stable building block, and they did not offer
any explanation for the high melting temperatures.
Traditionally, classical molecular dynamics (MD)
simulations have been used to understand the finite-0031-9007=04=92(13)=135506(4)$22.50data of sodium clusters are based on classical MD em-
ploying a variety of parametrized interatomic potentials
[7]. However, these attempts have fallen short of repro-
ducing the crucial characteristics observed experimen-
tally, such as the precise sizes at which maxima in the
melting temperatures occur. Quite clearly, for reproduc-
ing the experimental results a more realistic treatment of
interacting electrons is desirable. Recently, we have suc-
cessfully demonstrated the power of density functional
molecular dynamics (DFMD) by providing a detailed
explanation of the experimentally observed phenomena
of higher-than-bulk melting temperatures for tin clusters
[8]. In particular, we have shown that the covalent bond-
ing along with the existence of a highly stable tricapped
trigonal prism (TTP) subunit is responsible for the higher
melting temperature. For gallium clusters also, an
ab initio treatment is quite crucial for simulating the
finite-temperature behavior, especially since there is a
possibility of a change in the nature of the bonding.
In this Letter, we provide an explanation and insight
into the phenomenon of the higher-than-bulk melting
temperature recently observed in small gallium clusters
[5]. To this end we have carried out ab initio density
functional simulations over a wide range of temperatures
for the neutral clusters Ga17 and Ga13. We present the cal-
culated specific heat obtained via a multiple-histogram
(MH) analysis [9]. We also present a detailed analysis of
bonding in these clusters and contrast it with that of bulk.
In an earlier density functional calculation by Jones, the
bonds in small gallium clusters have been found to be
shorter than those between the lighter atoms in the same
main group, i.e., Al [10]. As we shall see, these clusters
indeed melt at a temperature substantially higher than
Tmbulk, mainly due to the formation of covalent bonds. 2004 The American Physical Society 135506-1
P H Y S I C A L R E V I E W L E T T E R S week ending
2 APRIL 2004VOLUME 92, NUMBER 13the local density approximation, as implemented in the
VASP package [11]. For Ga17, the MD calculations were
carried out for 23 temperatures, each of duration 75 ps, in
the range of 150  T  1100 K, which results in a total
simulation time of 1.65 ns. The resulting trajectory data
have been used to compute the ionic specific heat by
employing the MH method [9,12]. For all the calcula-
tions, we have used only sp electrons (4s2 and 4p1) as
valence electrons, taking 3d as a part of the ionic core
(represented by an ultrasoft pseudopotential). We have
verified that the d electrons do not significantly affect
the finite-temperature behavior and equilibrium geome-
tries by recalculating the equilibrium structures, and
performing three runs at finite temperature around the
melting region, with the d electrons treated explicitly as
valence electrons.
We begin our discussion by noting some interesting
features of the electronic structure of bulk Ga, which
has been investigated by Gong et al. [13]. The -Ga lat-
tice, which is stable at ambient pressure, can be viewed as
base-centered orthorhombic with eight atoms in the unit
cell. The peculiarity of this structure is that each atom
has only one nearest neighbor connected by a short bond
at a distance of 2:44 A(see Fig. 1). The six other neighbors
are at distances of 2.71 and 2:79 A, in two sets of three.
These six atoms lie on strongly buckled parallel planes
connected by the short bonds, as shown in Fig. 1. Elec-
tronic structure calculations by Gong et al. [13] reveal
this short bond to be covalent in nature. The density of
states shows a pseudogap, which has been related to this
covalent bond [14], and the weak bonding in the buckled
planes leads to an observed metallic behavior. Thus, two
kinds of bonds coexist in bulk Ga: one a molecular bond
between the nearest neighbors and the other a metallic
bond within the buckled planes.
Now we present and discuss some relevant features
observed in the equilibrium structures of Ga17. We have
relaxed many structures, randomly chosen from high-
temperature DFMD runs. In this way, we have found
more than 20 different equilibrium structures spanningFIG. 1. A part of the bulk structure of -Ga (not a unit cell).
It shows two buckled planes. The dark line joining the black
atoms corresponds to the interplanar covalent bond discussed
in the text.
135506-2an energy range of about 0.83 eV with respect to the
ground-state energy. In Fig. 2, we show some low-lying
structures relevant to the present discussion. A common
feature observed in all these geometries, except one
[Fig. 2(d)], is the presence of a trapped atom, that is, a
single atom contained within a cage formed by the re-
maining atoms. The lowest-energy structure that we have
found [Fig. 2(a)] is a highly asymmetric structure, which
can be thought of as formed out of a decahedron with
serious distortions and asymmetric capping. Interest-
ingly, this structure can also be viewed as composed of
two near planar rings, as discussed further below.
We have also analyzed the nature of bonding by em-
ploying the electron localization function (ELF) [15],
which is defined such that values approaching unity in-
dicate a strong localization of the valence electrons and
covalent bonding. The isosurface of the ELF for the
neutral Ga17 and charged Ga17
 are shown in Figs. 3(a)
and 3(b), respectively. A striking feature seen in these
figures is the existence of strong localized bonds giving
rise to two ringlike structures. Further, these rings are
also bonded to each other via the atoms at the edge of each
ring and with the trapped atom at the center. The exis-
tence of an isosurface of the ELF with such a high value
clearly indicates the covalent nature of the bonding. This
is also substantiated by examination of the corresponding
charge-density isosurface (not shown). Calculations of
the ELF for the excited isomers in Fig. 2 and for other
small Ga clusters show similar features. Generally, most
atoms have two covalent bonds in a roughly linear ar-
rangement, with a tendency to link neighbors together
into rings or ring fragments; extra covalent bonds on
some atoms then join these structures together. The bond-
ing here is thus seen to be in sharp contrast to the one
observed in the bulk -Ga, where, as discussed earlier,
only a single strong interlayer bond between two GaFIG. 2. The ground-state geometry and some of the the low-
energy structures of Ga17. The structures are arranged in
increasing order of the energy. (a) represents the lowest-energy
structure and (d) represents the highest-energy structure
studied. Energy differences E are in eV.
135506-2
1.4
v/
C
0)
P H Y S I C A L R E V I E W L E T T E R S week ending
2 APRIL 2004VOLUME 92, NUMBER 13atoms exists (see Fig. 1). An analysis of the bond lengths
reveals that each atom in the cluster has at least two near-
est neighbors at a distance of 2:5 A or less. Indeed, it is
this difference in bonding that is primarily responsible
for the higher melting temperature of the small clusters.
An examination of the molecular orbitals and the ei-
genvalue spectrum (not shown) brings out some notable
features. The eigenvalue spectrum is divided into two
groups, which are separated by about 1.18 eV. The lower
15 states forming the first group are the bonding states
formed out of atomic 4s orbitals. Almost all the upper
states are formed out of pure atomic p orbitals and show
no sp hybridization. The only exception to this is the
bonding between the trapped atom and its three nearest
neighbors, where a weak sp2 hybridization is observed.
This picture is also confirmed by a site-projected spheri-
cal harmonics analysis of the orbitals, which does not
show any significant mixing of s and p character in these
states. All the bonds seen are of predominantly 
 type,
formed out of atomic s and p orbitals. The lack of sp
hybridization explains the tendency to form covalent
bonds at approximately 180 or 90 angles, as observed
in Fig. 3.
The calculated specific-heat curve for Ga17 is shown in
Fig. 4. A clear peak is observed in the specific heat with a
maximum around 650 K, well above the bulk melting
point of 303 K. Following the discussion in Ref. [8], we
expect the statistical uncertainty in our peak position to
be up to 15%. Now, a novel multicollision induced disso-
ciation scheme has recently been used to measure the
caloric curve of small, charged Ga clusters [5]. For
Ga17
, no evidence was found for melting (in the sense of
a peak in the specific heat) over a temperature range 90–
720 K. Our simulations are consistent with this finding.
Note that there is likely to be some shift of the melting
temperature between the neutral and charged cluster.
While the thermodynamic simulation has been carried
out for neutral Ga17, calculations of the ELF in Ga17

reveal a similar network of covalent bonds [see Fig. 3(b)].
The ground-state geometry changes to a more symmetric
form (which is a low-lying isomer for Ga17), and the
HOMO-LUMO (highest occupied molecular orbital–
lowest unoccupied molecular orbital) gap increasesFIG. 3. The isosurface of ELF for (a) Ga17 at the value 0.68
and (b) Ga17 at the value 0.65.
135506-3from 0.76 eV for the neutral to 1.07 eV. The low-lying
isomers span an energy range of order 0.8 eV for both Ga17
and Ga17
. Therefore, we expect Ga17
 to have similar
melting properties to Ga17. The larger HOMO-LUMO
gap for Ga17
 may imply that it has a slightly higher
melting temperature.
Our specific-heat curve shows no premelting features
in the temperature range studied, and that the peak is
quite broad, as expected for the finite-sized systems. A
detailed examination of the ionic motion at different
temperatures sheds more light on the nature of melting.
Around 225 K, we observe the occurrence of the first
excited state [Fig. 2(b)]. As the temperature rises further,
the system visits a variety of isomers all of which contain
a trapped atom. It is only above 550 K that the isomer
shown in Fig. 2(d) is observed. Evidently, the peak in the
specific heat is associated with the diffusion of the
trapped atom out of the enclosing structure. Interest-
ingly, in the trajectories at all temperatures below
600 K, the trapped atom is seen to bond itself to atoms
in both rings. This confers stability on the caged struc-
ture. We have also carried out the analysis of the melting
properties via traditional parameters such as the root-
mean-square bond-length fluctuations and the mean
square atomic displacements (not shown). Their behavior
is consistent with the above observations.
To summarize, our ab initio MD simulations have
shown that the elevated melting temperature of Ga17 is
due mainly to the formation of covalent bonds. The
stability of the cluster is further enhanced by the role of
the caged atom. These observations should have implica-
tions for the melting characteristics of clusters of smaller
sizes, such as Ga13. The ground-state geometry of Ga13 is
decahedral, a more compact structure having a greater
average number of covalent bonds per atom than Ga17.
Further, our bonding analysis shows that the bonding is
strongly covalent, similar to Ga17. We therefore expect
this cluster to melt at a higher temperature than Ga17. To1.08
1.16
1.24
1.32
300 450 600 750 900 1050
C
an
on
ic
al
 S
pe
ci
fi
c 
H
ea
t (
C
Temperature (K)
FIG. 4. Normalized canonical specific heat of Ga17 cluster.
C0  3N  9=2kB is the zero temperature classical limit of
the rotational plus vibrational canonical specific heat.
135506-3
FIG. 6. The isosurface of ELF for Ga40 at the value 0.64.
1
1.2
1.4
1.6
1.8
400 700 1000 1300 1600
C
an
on
ic
al
 S
pe
ci
fi
c 
H
ea
t (
C
v/
C
0)
Temperature (K)
FIG. 5. Normalized canonical specific heat of Ga13 cluster.
P H Y S I C A L R E V I E W L E T T E R S week ending
2 APRIL 2004VOLUME 92, NUMBER 13verify this conjecture, we have carried out extensive
DFMD simulations for 30 different temperatures in the
range 40  T  1750 K, with a total simulation time of
about 2.7 ns. The resulting specific heat is shown in Fig. 5.
Indeed, the peak is around 1400 K, a much higher value
than the peak position of Ga17 or the bulk melting point.
The detailed analysis will be published elsewhere.
Finally, we note that Ga39
 and Ga40
 have been
measured to have a broad maximum in the specific heat
around 550 K [5]. Unfortunately, the large sizes of these
clusters prevent us from making a complete thermody-
namic study at this stage. However, we have found and
analyzed some low-lying equilibrium structures of Ga40.
We believe that a mechanism similar to that in Ga17 is
operative in Ga39
 and Ga40
. In Fig. 6 we show an
isosurface of the ELF for the value of 0.64 for Ga40.
The ringlike structures of covalent bonds are once again
clearly evident. However, it may be noted that at this
value of the ELF no contours are seen between the inner
core atoms and the outer surface, and not all the atoms on
the surface are bonded. Therefore, it is not unreasonable
to expect this cluster to melt at a somewhat lower tem-
perature than Ga17, but still higher than that of the bulk.
In conclusion, we have carried out extensive density
functional thermodynamical simulations on Ga17 and
Ga13 with the aim of understanding the observed
higher-than-bulk melting temperatures. The analysis of
the specific-heat curve indicates the melting temperatures
(defined as the peak of the specific-heat curve) to be
around 650 and 1400 K for Ga17 and Ga13, respectively.
This result is consistent with the recent experimental
observations of Breaux et al. [5]. We find a significant
change in the nature of bonding between bulk Ga and
small Ga clusters. The strong covalent bonds in the small
clusters, along with the stabilizing role of the trapped
atom in Ga17, are responsible for the higher-than-bulk
melting temperatures. While the structural details for Sn
and Ga clusters are very different, the common feature135506-4between these two systems is thus seen to be the develop-
ment of strong covalent bonding in the small clusters.
One of us (S. C.) acknowledges financial support
from CSIR (New Delhi). It is a pleasure to acknowledge
C-DAC (Pune) for providing us with supercomputing
facilities.[1] M. Schmidt, R. Kusche, Th. Hippler, J. Donges,
W. Kronmüller, B. von Issendorff, and H. Haberland,
Phys. Rev. Lett. 86, 1191 (2001).
[2] A. A. Shvartsburg and M. F. Jarrold, Phys. Rev. Lett. 85,
2530 (2000).
[3] M. Schmidt and H. Haberland, C. R. Physique 3, 327
(2002); M. Schmidt, R. Kusche, W. Kronmüller,
B. von Issendorff, and H. Haberland, Nature (London)
393, 238 (1998).
[4] P. Pawlow, Z. Phys. Chem. (Leipzig) 65, 1 (1909);
Ph. Buffat and J.-P. Borel, Phys. Rev. A 13, 2287 (1976).
[5] G. A. Breaux, R. C. Benirschke, T. Sugai, B. S. Kinnear,
and M. F. Jarrold, Phys. Rev. Lett. 91, 215508 (2003).
[6] R. S. Berry, Int. J. Mod. Phys. B 6, 3695 (1992); D. J.
Wales, Mol. Phys. 78, 151 (1993).
[7] F. Calvo and F. Spiegelmann, J. Chem. Phys. 112, 2888
(2000); N. Ju and A. Bulgac, Phys. Rev. B 48, 2721
(1993).
[8] Kavita Joshi, D. G. Kanhere, and S. A. Blundell, Phys.
Rev. B 66, 155329 (2002); 67, 235413 (2003).
[9] A. M. Ferrenberg and R. H. Swendsen, Phys. Rev. Lett.
61, 2635 (1988); P. Labastie and R. L. Whetten, Phys.
Rev. Lett. 65, 1567 (1990).
[10] R. O. Jones, J. Chem. Phys. 99, 1194 (1993).
[11] Vienna ab initio simulation package, Technische
Universität Wien, 1999; G. Kresse and J. Furthmüller,
Phys. Rev. B 54, 11169 (1996).
[12] D. G. Kanhere, A. Vichare, and S. A. Blundell, Reviews in
Modern Quantum Chemistry, edited by K. D. Sen (World
Scientific, Singapore, 2001).
[13] X. G. Gong et al., Phys. Rev. B 43, 14 277 (1991).
[14] V. Heine, J. Phys. C 1, 222 (1968);V. Heine and D.Weaire,
Solid State Phys. 24, 249 (1970).
[15] B. Silvi and A. Savin, Nature (London) 371, 683 (1994).135506-4


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Why do gallium clusters have a higher melting point than the bulk?

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