T. Goto, Y. Ito / Journal of Physics and Chemistry of Solids 66 (2005) 418–421
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chlorides. Then, thus prepared liquid tin film was used as
an anode and potentiostatic electrolysis of the anode was
conducted to obtain tin nitride film. After the electrolysis,
the products were analyzed by means of X-ray photo-
electron spectroscopy (XPS) and photoluminescence
measurement (PL). Through the experimental results, we
clarified the relationships between tin nitrides and electro-
lytic conditions.
2. Experimental
All experiments were conducted in an argon atmosphere
using a glove box with a continuous gas-refining instrument
(Japan Pionics Co., Ltd: MBN-R-07). The experimental
setup used was the same as previously reported [6,7]. The
solvent was a binary eutectic mixture of LiCl–KCl prepared
from vacuum dried reagent grade chemicals (Wako Pure
Chemical Co., Ltd). Li3N (Wako Pure Chemical Co., Ltd)
was added directly into the melt as a nitride ion source.
SnCl2 was added directly into the melt as bivalent tin cation
source. An electrochemically polished nickel plate (The
Nilaco Co., Ltd: 99.99%) was used as the working electrode.
Aluminum was used as the counter electrode. The reference
electrode was a Li–Al alloy in the state coexisting (aCb)
phase, and prepared electrochemically from an aluminum
wire (20 mm!: 1 mm, The Nilaco Co., Ltd: 99.99%). The
potential of this electrode shows the equilibrium potential of
the following reversible reaction [8]:
Fig. 1. A cyclic voltammogram of Ni in LiCl–KCl–SnCl2 at 673 K.
prepare a tin film that stably maintains a liquid film state
with wide area in molten chlorides. For this purpose,
the electrochemical formation of tin in molten LiCl–KCl
was carried out.
Before conducting electrochemical formation of tin, the
electrochemical behavior of tin ions on a nickel electrode in
LiCl–KCl was studied by means of cyclic voltammetry.
Fig. 1 shows a cyclic voltammogram of nickel in LiCl–KCl–
SnCl2 (0.1 mol%) at 673 K. One cathodic wave is observed
at 2.2 V, which corresponds to the formation of metallic tin
according to the following reaction:
SnðIIÞ C2eK Z Sn
(1)
The corresponding anodic wave is attributable to the
dissolution of tin. Further electrochemical measurement
was carried out by means of chronopotentiometry. Fig. 2
shows a chronopotentiogram of Ni in LiCl–KCl–SnCl2 at
673 K. While galvanostatic electrolysis was conducted at
K10 mA, the plateau potential of 2.12 V corresponds to
the formation of a liquid tin. The following potential
plateau of 2.16 V corresponds to the coexistence of nickel–
tin alloy phase [10] during conducting galvanostatic
electrolysis at 0.5 mA. Based on the results, potentiostatic
electrolysis was conducted at 1.9 V, which potential was
negative enough to form metallic tin on a nickel substrate.
AlðaÞ CLiC CeK Z 2Li0:5Al0:5ðbÞ
A dynamic reference electrode using electrochemically
deposited lithium was used to correct the potential
measured by the Li–Al alloy reference electrode. All
potentials in this paper are referred to this potential and
shown as (V vs. LiC/Li) [9]. Electrochemical measure-
ments were conducted using a potentio/galvanostat
combined with a function generator (Hokuto Denko Co.,
Ltd: HZ-3000). Measurements of surface chemical states
and depth profiles were performed by an X-ray photo-
electron spectroscopy (XPS) (Shimadzu Co., Ltd: ESCA-
3200-01) using Mg Ka line as the X-ray source. The
measurement of the nitrogen concentration profiles was
also conducted by an electron probe microanalyser
(EPMA) (Horiba Co., Ltd: EMAX-2200). Photolumines-
cence (PL) measurement was carried out using a He–Cd
laser of 325 nm at room temperature.
3. Results and discussion
3.1. Electrochemical formation of tin from molten LiCl–KCl
In order to obtain a tin nitride film by means of the
electrochemical nitriding of liquid tin, it is necessary to
Fig. 2. A chronopotentiogram of Ni in LiCl–KCl–SnCl2 at 673 K.