Development of Removable Hollow Cathode Discharge Apparatus for Sputtering Solid Metals

A hollow cathode discharge cell has been developed for a variety of sample phases. To make the experimental apparatus compact, we have adopted DC discharge, and the discharge cell was inexpensively constructed for replacement with commercially available vacuum parts. 1e most distinctive attribute of the developed cell is the double structure of the cathodes. 1e occurrence of sputtering resulted in the metal atom in gas phase. With Ar buffer gas, the favorable condition of laser absorption spectroscopy for the gas phase sample was investigated.


Introduction
A hollow cathode concentrates electron density in the center of the cathode.As a result, it is expected that in this region, the density of excited atomic species is highest [1]. is geometry is suitable for laser spectroscopy, and consequently, hollow cathode discharge cells have already been made commercially available [2].Paschen first developed this structure and Jones and Walsh [3] and Grimm [4] improved it for atomic absorption spectroscopy, in particular for the purpose of isotope spectroscopy.In addition, many articles referencing the technique have been published, such as in laser frequency calibration and absorption spectroscopy of Li [5], Fe [6], U [7], and molecules [8].e excited noble gas atoms in discharge collide with other atoms, the transfer of energy causing excitation of electrons.Additionally, electrons in a discharge may also cause atomic excitation.It does not require multiple laser sources for excitation like in Resonance Ionization Spectroscopy (RIS).In addition, excited atomic species or ions of noble gases can be generated easily and may be used to produce a vapor of solid metal samples by way of sputtering, which is the collision of the noble gas ions with the metal electrodes resulting in the ejection of the metal atoms.Sputtering as a technique is widely used for fabrication of multithin films in material science, with particular merit being that it can produce the required atomic vapor with a minimum chemical pretreatment of the donor material surface.
erefore, the use of this method in conjunction with discharge spectroscopy provides an advantage over other popular spectroscopic methods, such as Inductively Coupled Plasma Atomic Emission Spectroscopy (ICP-AES), which do require extensive pretreatment.Various methods are utilized for vaporizing samples such as direct current (DC) [9], radio frequency (rf ) [10], and microwave discharges [11].Mass spectrometry like Secondary Ion Mass Spectrometry (SIMS) [12] makes use of sputtering for vaporization of a sample.
e experimental setup required is generally large; however, DC sputtering is small and low cost.
In this work, we describe the development of a hollow cathode glow discharge cell capable of analyzing a variety of samples, a property which is difficult for commercially available items to achieve because of their sealed structure.
ere are a few publications [5][6][7][8] reporting discharge cells capable of the analysis of one specific element.However, our discharge cell may be able to be applied to the analysis of multiple samples/elements thanks to the double cathode structure, wherein the inner cathode is demountable.Our discharge cell is expected to be able to analyze not only gases, but also liquid residues on the electrode, and solid metals used as the electrode in bulk form.In addition, the memory e ect (e ects of the residues of previous experiments) can be disregarded in applying the apparatus to chemical analysis, due to the replaceability of the inner cathode.As examples of the apparatus capability in regard to solid metals, a tungsten hollow cathode and liquid residue, mixed elements ICP standard sample, are shown to be e ective as a metal vapor source without additional chemical pretreatment.Subsequently, the various isotopes of the excited noble gas could be observed in spectroscopy with a high-resolution CW laser.Out of the various kinds of discharge techniques, we employed DC glow discharge.Glow discharge takes place in low-pressure plasmas where the temperature of the ions is di erent from that of the electrons.It is less damaging to components than arc discharge, and the noble gas density for inducing discharge is low, which is ideal for optical spectroscopy.

Experimental Setup
e discharge cell was designed to consist of an electrically insulated, transparent Duran NW40 cross (Evac, 33.040007.171.740).For spectroscopy, low-absorption transparent view ports (Evac, 32.123.840)were employed.An electric current feed through ange (Kyo-Cera, N405BR2) for two MHV terminals with long ceramic insulators to avoid inappropriate discharge between the feed through and the ange was used to introduce the electrical connections.
e pressure in the cell was monitored with a capacitance gauge (Canon-Anelva, M-342DG-13) with range from 10 Pa to atmospheric pressure.Air was evacuated by a rotary pump (Pfei er Vacuum, 2005 SD), and the discharge bu er gas (Ar or Ne) was supplied via a bellows valve (Swagelok, SS-4BG).Isolation of the cell from the pumping pipeline was achieved by a diaphragm valve (VAT, 22032-KA01) (Figure 1).e cathode electrodes have a doubled structure (Figure 2). is structure enables the investigation of various samples simply by changing the inner cathode.
ey are made of titanium (inner) and nichrome (outer), and their sizes are as follows: inner cathode (right upwarddashed in Figure 2, TI-45590, purchased from Nilaco, Tokyo, Japan) has 4.1 mm inner diameter (ID), 5.1 mm outer diameter (OD), and 27 mm in length.e dimension of the outer cathode (orange solid color in Figure 2) is 5.2 mm (ID), 10 mm (OD), and 27 mm in length.e cathode edges were not rounded to prevent surface discharge.Titanium was employed because of its low cost and high heat durability.Nichrome was employed because of its higher durability against discharge ablation compared to stainless steel, based on our experience.e external surface of the hollow cathode (left upward-dashed in Figure 2) is insulated by glass.e dimensions of the glass components are ID (10.2 mm), OD (14 mm), and the length (28 mm).
e glass is supported by the cathode standing rod.e anode is made of stainless steel and its size is 7 mm (ID), 8 mm (OD).e distance between the electrodes is approximately 3-4 mm.To allow for continuous discharge, a ballast resistor of 1 kΩ is connected to the plasma cell in series.A voltmeter was also connected across the resistor to monitor the resistor voltage.e voltage between the electrodes was calculated from the voltage of the electronic power supply minus that of the ballast resistor.
A Ti : S laser (Coherent, 899-21) excited by a diode pumped solid-state laser (Coherent, Verdi10) was employed for laser absorption spectroscopy (Figure 3).Frequency calibration was achieved with a Fizeau type interference wavemeter (High Finesse, WSU-30).Light transmitted through the cell was observed with a photodetector.High-sensitivity detection was obtained by a Lock-in-Ampli er (Stanford Research Systems, SR830) and optical-chopper (Stanford Research Systems, SR540).For emission spectroscopy, a compact spectrometer (Ocean Optics, Flame-S, wavelength resolution: 1.02 nm, observable range: 190-880 nm, cumulative time: 1 ms- 2 Journal of Spectroscopy 65 s) was used to monitor chemical species, such as atoms and molecules, in the discharge.e control and data acquisition was conducted via LabVIEW (National Instruments) and VBA (Microsoft).

Results
Sputtering is e cient in the abnormal glow region [13].With this method, solid samples may be vaporized into single atoms even if they are present in the sample as chemical compound constituents.As examples, the emission spectra of sputtering of solid tungsten (Figure 4) and liquid residue containing several elements (Figure 5) were observed.
e liquid residue sample was dropped onto the electrode and dried with infrared lamp heating.
anks to this technique, metals of nonneutral atom were made into those of neutral atom without chemical reduction treatment.Although the elemental assignment of the mixed sample (Merck, ICP multielement standard IV) was successful on 17 elements, through comparison with the observed spectrum of pure element or spectra database [14], 6 elements Ag, Bi, Cd, Co, Li, and Tl were not able to be assigned, due to the interference with other signals.As an example, in the case of Li, the wavelength of the distinctive peaks is 670.776nm and 670.791 nm, but there are emissions close to these values: Ne emission at 671.704 nm and Ar at 669.887 nm.
erefore, a spectrometer resolution of less than 0.5 nm would be required to resolve the Li signals.As Figure 5 shows, the metals in liquid residue may exist as the neutral atoms, even if their metal valence are between one and three in solution.
e transitions used in the laser absorption spectroscopy experiment are 2p 5  6 shows the Ne absorption spectrum.From Voigt tting, the isotope shift of Ne-20 (90% abundance) and Ne-22 (10%) was estimated to be 0.92 GHz.
e intensities of absorption for excited species of Ar were investigated in a continuous ow of Ar and also for a sealed cell of Ar.
e "sealed mode" was the condition under which the bellows valve and the diaphragm valve were closed."Flow mode" is the name given to the condition where the experiment was performed with the intake produced by rotary pump and with the gas cylinder regulator open.Ar absorbance was measured in pressure range 100-400 Pa with 20 mA (Figure 7).At less than 100 Pa, discharge was not observed, due to the atomic density being too low for discharge to occur.In the continuous gas ow mode, atoms in the excited state are continually replaced with atoms in the ground state, due to the ow of the gas.e concentration of atoms in highly excited states at the cathode was lower in the ow mode.
e ratio of atoms in the lower state to higher state is di erent between the ow mode and sealed mode.It resulted in larger absorbance in ow mode as shown in Figure 7.In addition, the dependency of absorbance was investigated for various pressures and currents (Figure 8).It shows higher current results in a larger absorbance.e increase of current caused an increase in electron density and therefore increased probability of the excitation of gases in discharge.From this increase in probability, the relationship between current and absorbance was subsequently identi ed.In addition, the increase of the pressure decreased the density of excited atomic gases.Consequently, we can conclude that the relation between gas pressure and absorbance is that absorbance decreases with pressure increase.From Figures 7 and 8, the preferable conditions for higher absorption are at lower pressure and higher current for this transition.

Conclusion
We developed a hollow cathode cell, which can be used to observe absorption and emission of noble gases with isotope shift resolution under illumination by laser light.By discharge technique, tungsten and mixed liquid residue were sputtered to atoms, which can be utilized as the neutral metal atom vapor sources.e inner cathode of the double cathode structure is demountable and can allow for the introduction of a variety of sample phases, such as gases, liquid residues, or metal solids.For a metal vapor source, preferable sputtering conditions were investigated with various pressures of Ar and Ne under 4 Journal of Spectroscopy discharge.In the future, we intend to further investigation of laser absorption spectroscopy using the experiment of apparatus.
Data Availability e data used to support the ndings of this study are available from the corresponding author upon request.

Figure 1 :Figure 2 :
Figure 1: Diagram of the plasma experimental setup.

Figure 7 :Figure 8 :
Figure 7: Absorbance of Ar in owing gas and sealed cell cases at 20 mA.