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Journal of Crystal Growth
journal homepage: www.elsevier.com/locate/jcrysgro
Tl
2
HfCl
6
and Tl
2
ZrCl
6
: Intrinsic Tl-, Hf-, and Zr-based scintillators
R. Hawrami
a,
⁎
, E. Ariesanti
a
, V. Buliga
a
, A. Burger
a
, S. Lam
b
, S. Motakef
b
a
Fisk University, Nashville, TN 37208, USA
b
CapeSym, Inc., Natick, MA 01760, USA
ARTICLE INFO
Communicated by R.S. Feigelson
Keywords:
B2. Intrinsic scintillator
A1. Cubic structure
B2. Tl-, Hf-, Zr-based scintillator
B2. High density scintillator
B2. Bright scintillator crystals
B2. Good proportionality
ABSTRACT
The re-discovery of Cs
2
HfCl
6
(CHC) as a scintillator has lately generated much interest in this material and its
family, which belongs to the K
2
PtCl
6
cubic crystal structure [1]. CHC is an intrinsic scintillator that is non-
hygroscopic, has no self-radioactivity, provides good energy resolution, and has good non-proportionality. In
this paper we are reporting growth and scintillation properties of two new and Tl-, Hf- and Zr-based compounds
of Tl
2
HfCl
6
and Tl
2
ZrCl
6
, with physical densities of 5.1 g/cm
3
and 4.5 g/cm
3
, respectively and effective atomic
numbers (Z
eff
) of 71 and 69, respectively. Samples from successfully grown 16 mm diameter boules were cut,
processed, and characterized for their scintillation and radiometric properties. Energy resolutions of 3.7%
(FWHM) for THC and 3.4% for TZC (FWHM) at 662 keV are measured. Primary luminescence decay times of
1.1 μs and 2.3 μs, for Tl
2
HfCl
6
and Tl
2
ZrCl
6
, respectively, as well as good proportionality for both materials have
been observed.
1. Introduction
Widespread use of scintillators as gamma-ray detectors is largely
generated by their tunable properties and extensive availability.
Currently there are needs for scintillators with targeted properties such
as high light output, high stopping power (Z
eff
), fast decay time, good
linearity and low cost. A rediscovered family of scintillators, Cs
2
HfCl
6
[1], has recently been in one of the materials in the forefront of new
scintillator development for gamma-ray detectors. CHC was re-dis-
covered and reported as an example of a little-known class of non-hy-
groscopic compounds having the generic cubic crystal structure of
K
2
PtCl
6
[1]. Since its re-discovery as a new non-hygroscopic, intrinsic
scintillator with a simple cubic crystal structure, several papers have
reported their studies on their attractive properties as well as growth
challenges. In an initial study CHC scintillation was reported to be
centered at 400 nm, with a principal decay time of 4.4 μs and a light
yield of up to 54,000 photons/MeV (when compared to BGO), and
energy resolution of 3.3% at 662 keV using a 0.65 cm
3
cubic sample [2].
Another study on crystal growth and behavior CHC and its variant,
Cs
2
HfCl
4
Br
2
(CHCB), also reported a clear CHC sample with a light yield
and energy resolution of 30,000 ph/MeV (when compared to NaI:Tl)
and 3.3%, respectively, and decay components of 0.39 and 3.9 μs. A
sample of CHCB with a secondary phase present in the core had a light
yield and energy resolution of 18,600 ph/MeV and 4.4%, and with
decay components of 0.38 and 2.0 μs for CHCB. Both CHC and CHCB
showed minimal moisture sensitivity [3].
Recently Tl
2
HfCl
6
and Tl
2
ZrCl
6
, compounds belonging to a new sub-
family based on substitution of Tl
+
for Cs
+
in CHC, have been pub-
lished [4]. These compounds, similarly to CHC and CHCB, were also
grown by the vertical Bridgman–Stockbarger method. The Tl
+
ion
substitution increases both the density (see Table 1) as well as the ef-
fective atomic number Z
eff
(see Table 1 and [4]), factors which directly
determine x-ray/γ-ray detection efficiency of materials. Both Tl
2
HfCl
6
and Tl
2
ZrCl
6
crystals showed an intrinsic emission band peak between
450 and 470 nm under UV light and X-ray excitations. Their reported
energy resolutions at 662 keV were 17.7% for Tl
2
HfCl
6
and 5.6% for
Tl
2
ZrCl
6
. Their reported scintillation decay times are 288 and 6340 ns
for Tl
2
HfCl
6
, while for Tl
2
ZrCl
6
696 and 2360 ns [4]. Our paper is re-
porting on initial growth of Tl
2
HfCl
6
and Tl
2
ZrCl
6
single crystal boules
with improved radiometric and scintillation properties. Compared to
previously published papers on these materials, with respect to crystal
size and scintillating performance, our results demonstrate successful
crystal growth runs resulting in superior crystal quality.
2. Experimental Methods
The crystal growth process started by loading stoichiometric
amounts of starting materials respectively according to compound (TlCl
with 99.99% and HfCl 99.9% for Tl
2
HfCl
6
and TlCl with 99.99% and
ZrCl 99.9% for Tl
2
ZrCl
6
) into 16 mm diameter ampoules, completed
https://doi.org/10.1016/j.jcrysgro.2019.125316
Received 7 September 2019; Received in revised form 15 October 2019; Accepted 21 October 2019
⁎
Corresponding author.
E-mail addresses: drh1980@gmail.com, rhawrami@fisk.edu (R. Hawrami).
Journal of Crystal Growth 531 (2020) 125316
Available online 22 October 2019
0022-0248/ © 2019 Elsevier B.V. All rights reserved.
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