Process for Manufacturing Single-Crystal Fiber
20240410081 ยท 2024-12-12
Inventors
Cpc classification
C30B29/28
CHEMISTRY; METALLURGY
C30B15/22
CHEMISTRY; METALLURGY
C30B13/08
CHEMISTRY; METALLURGY
International classification
C30B29/28
CHEMISTRY; METALLURGY
Abstract
The present disclosure provides a method for manufacturing a Nd:YAG single crystal fiber exhibiting a radial concentration distribution where the Nd concentration reaches a maximum at a central axis of the single crystal fiber. The method for manufacturing a Nd:YAG single crystal fiber according to the present disclosure involves: preparing a source material having a rod shape and containing a YAG single crystal or polycrystal, Nd, and Ca; melting an end of the source material to form a molten zone; and bringing the molten zone into contact with a seed crystal and pulling up the seed crystal to grow the single crystal fiber.
Claims
1. A method for manufacturing a single crystal fiber of Yttrium Aluminum Garnet (YAG) containing neodymium (Nd), the method comprising: preparing a source material having a rod shape and containing a YAG single crystal or polycrystal, Nd, and calcium (Ca); melting an end of the source material to form a molten zone; and bringing the molten zone into contact with a seed crystal and pulling up the seed crystal to grow the single crystal fiber.
2. The method for manufacturing a single crystal fiber according to claim 1, wherein a second ratio is 0.47 times or more a first ratio and is 0.08 or less where the first ratio represents a ratio of the number of Nd atoms contained in the source material to the number of yttrium (Y) atoms contained in the YAG single crystal or polycrystal and the second ratio represents a ratio of the number of Ca atoms contained in the source material to the number of Y atoms contained in the YAG single crystal or polycrystal.
3. The method for manufacturing a single crystal fiber according to claim 1, wherein the source material has a YAG single crystal or polycrystal as a mother phase and contains Nd and Ca inside the mother phase.
4. The method for manufacturing a single crystal fiber according to claim 1, wherein the source material comprises a base and an oxide layer formed on an outer surface of the base.
5. The method for manufacturing a single crystal fiber according to claim 2, wherein the source material has a YAG single crystal or polycrystal as a mother phase and contains Nd and Ca inside the mother phase.
6. The method for manufacturing a single crystal fiber according to claim 2, wherein the source material comprises a base and an oxide layer formed on an outer surface of the base.
7. The method for manufacturing a single crystal fiber according to claim 3, wherein the source material comprises a base and an oxide layer formed on an outer surface of the base.
Description
BRIEF DESCRIPTION OF DRAWINGS
[0016]
[0017]
[0018]
[0019]
[0020]
[0021]
[0022]
DESCRIPTION OF EMBODIMENTS
[0023] Hereinafter, various embodiments of the present disclosure will be described in detail with reference to the drawings. The same or similar reference numerals denote the same or similar components, and repetitive explanation thereof may be omitted. The following description is an example, and some configurations may be omitted, modified, or implemented together with additional configurations without departing from the gist of an embodiment of the present disclosure.
[0024] A method for manufacturing a Nd:YAG single crystal fiber according to the present disclosure employs the LHPG technique as similar to a method in the related art. However, the method according to the present disclosure differs from the method in the related art in that a separate element from Nd is added to a YAG source material and that a fluid behavior of a melt in a molten zone 12 is changed as illustrated in
[0025] As described above, a method 20 for manufacturing a Nd:YAG single crystal fiber 14 by the LHPG technique in the related art causes a radial concentration distribution where the Nd concentration reaches a maximum in an area away from a central axis of the single crystal fiber 14 due to a density gradient in the molten zone 12 according to a segregation coefficient of Nd in a YAG crystal. However, adding an additional element having a small segregation coefficient and small atomic weight makes it possible to form a molten zone while a melt is maintained to have a density equal to that of a source material, thereby preventing a density gradient of the melt. In other words, it is possible to manufacture by the LHPG technique a Nd:YAG single crystal fiber that exhibits a radial concentration distribution where the Nd concentration reaches a maximum at a central axis of the single crystal fiber 14.
[0026] An example of the additional element satisfying such a condition includes calcium (Ca). Hereinafter, conditions of Ca to be added to Nd:YAG will be described in detail.
[0027] Ca-doped Nd:YAG is represented by the chemical formula Nd.sub.3xCa.sub.3yY.sub.3(1-x-y)Al.sub.5O.sub.12 where x represents a ratio of the number of Nd atoms to the number of Y atoms contained in YAG and y represents a ratio of the number of Ca atoms to the number of Y atoms. In the Ca-doped Nd:YAG, atomic weights of the constituent atoms are Y: 88.91, Al: 26.98, 0:16.00, Nd: 144.24, and Ca: 40.08, and a molecular weight S (x, y) of the Ca-doped Nd:YAG is represented by (Formula 1).
[0028] A volume change of a YAG melt due to additive elements (Nd and Ca) in YAG is of little significance, and S (x, y) in (Formula 1) is an effective parameter corresponding to the density.
[0029] In regard to a segregation coefficient k.sub.eff, it is known that Nd has a segregation coefficient K.sub.eff,Nd=0.21, and Ca has a segregation coefficient K.sub.eff,Ca=0.1 (for example, see Non Patent Literatures 2 and 3). Therefore, the additive elements Nd and Ca in the melt have concentrations of x/k.sub.eff,Nd=x/0.21 and y/k.sub.eff,Ca=y/0.1, respectively.
[0030] Assume that a Ca-doped Nd:YAG single crystal fiber is being grown (stably grown) by the LHPG technique based on the concentrations. A condition where the density of a newly molten melt becomes equal to or larger than that of a previously formed melt is represented by (Formula 2).
[0031] Therefore, when each value is plugged in (Formula 1) and (Formula 2), a condition that causes convection similar to convection of an additive-free melt is represented by (Formula 3).
[0032] However, in a case where YAG is doped with another element (for example, Ca), excessive addition of Ca increases free energy of a YAG crystal system, and a crystal structure cannot be maintained. Furthermore, instead of cation sites of Y, the amount of Ca between lattices increases, which may cause YAG to be amorphous or may cause the added Ca to be phase separated in the state of calcium oxide (CaO). In other words, the method for manufacturing a Nd:YAG single crystal fiber according to the present disclosure places an upper limit on the amount of Ca added to YAG.
[0033] In a case where a YAG crystal is doped with Ca, as similar to Nd, Ca substitutes for a Y cation site in YAG, and it is known that adding Ca as Cao in an amount of about 8 at. % makes it possible maintain a structure of the YAG crystal (for example, see Non Patent Literature 5). In CaO doping, it is known to add silicon (Si) to keep electrical neutralization (see, for example, Non Patent Literature 5). In this case, Si substitutes for a Al site, and the same number of Al atoms as the number of Si added is reduced from a raw material. Since Si has an effective ionic radius smaller than that of Al, a segregation coefficient of Si relative to YAG is approximately 1 and have no effect on convection of a melt.
[0034] From the above description, a ratio of the number of Ca atoms to be added to YAG to the number of Y atoms (corresponding to y described above) is 0.08 to 1 at a maximum. Taking this upper limit into account in (Formula 3) derives (Formula 4). This (Formula 4) represents a range in amount of Ca to be added in the present disclosure.
[0035] From the above description, manufacturing a Nd:YAG single crystal fiber by the LHPG technique under the condition that satisfies (Formula 4) enables the Nd:YAG single crystal fiber to exhibit a concentration distribution where the Nd concentration reaches a maximum at a central axis.
[0036]
[0037] In this manner, according to the present disclosure, it is possible to manufacture by the LHPG technique a Nd:YAG single crystal fiber exhibiting a radial concentration distribution where the Nd concentration reaches a maximum at a central axis of the fiber. Accordingly, as compared with a Nd:YAG single crystal fiber manufactured by a technique in the related art, the Nd:YAG single crystal fiber manufactured by the method for manufacturing a Nd:YAG single crystal fiber according to the present disclosure easily achieves oscillation in a fundamental transverse mode and enables a high-efficient laser oscillator and optical amplifier.
[0038] Although the method for manufacturing a Nd:YAG single crystal fiber according to the present disclosure employs a source material having a configuration different from one used in the method in the related art, both methods are the same in employing the LHPG technique. Accordingly, there is no need to thoroughly change the existing manufacturing process, which offers an advantage of maintaining an existing production line.
First Embodiment
[0039] Hereinafter, a first embodiment of the present disclosure will be described in detail with reference to the drawings. In this embodiment, a source material used in the LHPG technique has a YAG single crystal or polycrystal containing Nd and Ca as additive elements.
[0040]
[0041] The source material 17 is prepared by, for example, melting, sintering, element diffusion, ion implantation by ion beams but is not limited in manufacturing method.
[0042]
[0043] As described above, in the Nd:YAG single crystal fiber manufactured by this method, the addition of Ca prevents a density gradient of a melt, and a molten zone 12 takes on an aspect as illustrated in
Second Embodiment
[0044] Hereinafter, a second embodiment of the present disclosure will be described in detail with reference to the drawings. In this embodiment, a source material used in the LHPG technique has an oxide layer on its outer surface.
[0045]
[0046] The oxide layer 72 is formed on the outer surface of the base 71 by, for example, but is not limited to, a physical vapor deposition technique such as vacuum vapor deposition and magnetron sputtering, a chemical vapor deposition technique such as plasma CVD and photo CVD, a liquid phase growth technique such as plating and sol-gel process, a thermal spraying technique such as flame spraying and plasma spraying, or sintering such as hot isostatic pressing and spark plasma sintering.
[0047] Manufacturing a Nd:YAG single crystal fiber 14 by the method illustrated in
[0048] In this embodiment, for example, the base 71 of the source material 70 employs Nd:YAG and the oxide layer 72 employs Cao, but the materials are not limited to this combination. For example, the base 71 may employ YAG containing Ca as an additive element (Ca:YAG) and the oxide layer 72 may employ neodymium oxide (Nd.sub.2O.sub.3). The additive elements (Nd and Ca) of YAG may be contained in either the base 71 or the oxide layer 72.
[0049] Alternatively, the oxide layer 72 may be formed on an outer surface of the source material 17 described in the first embodiment, and the resultant may be employed as the source material 70.
[0050] However, in any embodiment, amounts of Nd and Ca in the entire source material 70 are required to satisfy (Formula 4) as described above.
INDUSTRIAL APPLICABILITY
[0051] Unlike the related art, the method for manufacturing a single crystal fiber according to the present disclosure enables manufacturing of a Nd:YAG single crystal fiber that exhibits a concentration distribution where the Nd concentration reaches a maximum at a central axis. Nd:YAG single crystal fibers having such a concentration distribution easily achieve oscillation in a fundamental transverse mode and are expected to be employed in laser oscillators and optical amplifiers.