★★★ ＜第 21 回知的財産翻訳検定試験【第 10 回英文和訳】＞ ★★★
≪１級課題 -電気・電子工学-≫【解答にあたっての注意】
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４．課題は３題あります。それぞれの課題の指示に従い、３題すべて解答してください。

問１）

次の英文は、特許明細書の「従来技術」に関する記載です。日本語に訳して下さい。

Typically, when a software developer is writing code, thedeveloper will compile and execute the code in a debugging mode.
A debugging mode may allow the developer a view into how thecode is functioning during execution. When code is executed ina debugging mode, the developer can typically: view variablevalues during execution, set breakpoints at which execution of
the code will halt until the developer triggers continued
execution, and/or step through execution of the code on aline-by-line basis. Such an arrangement may work well when thecode is being compiled, debugged, and/or executed at a computer
system local to the developer. In conventional arrangements,a choice between execution of code either entirely in a
debugging mode (that permits debugging functionality) or aruntime mode (that conventionally does not permit debugging
functionality) may need to be made. Such a choice may be easily
made by the developer when he is the only person using thecomputer system. Further, when a developer has code that isdesired to be debugged, the developer may only be interested
in debugging a portion of the code, while allowing the remainderof the code to execute without debugging functionality.

問２）

次の英文は、特許明細書の「発明の実施の形態」に関する記載です。添付した図1

面（ＦＩＧ．１、ＦＩＧ．２）も参照して、日本語に訳して下さい。

Board 100 includes a printed circuit board substrate 102
made of a material that is flexible in the longitudinal
direction so that it may be bent from the relaxed state shownin FIG. 1 into a radius to match the radius of a reel strip ina mechanical reel-type game. An example of a bent condition ofboard substrate 102 is shown in FIG. 2. Referring again to FIG.
1, twenty-four transverse rows of LEDs 104 (which may be single
color or multi-color LEDs) are mounted on the substrate 102.
The LED rows are staggered to allow closer spacing between rows
and because the closer spacing allows for more even lighting
by using half the LEDs. Board 100 includes eight attachmentopenings 106 which each represent an attachment or mounting
point at which the board may be mounted to a bracket. Each ofthe four lowermost openings 106 shown in FIG. 1 are located ina different respective corner of a rectangular light-supporting
region of substrate 102. LEDs 104 are mounted in the rectangularlight-supporting region of substrate 102. In one implementation,
each LED 104 is individually controllable. Other forms of theinvention may control each row of LEDs 104 as a unit.

23FIG. 24問３）次の英文は、特許明細書のクレーム（請求項）です。日本語に訳して下さい。なお、翻訳に当っては、クレームの後に記載している実施の形態の記載（抜粋）及び図面を参照して下さい。
1. A laser comprising:a pumping light source which emits an optical pumping
beam; anda laser resonator including an input mirror opticallycoupled to the pumping light source for receiving and passing
therethrough the optical pumping beam, an output mirror, alasant material, and a nonlinear optical material,
the lasant material being a material which lases in
response to the optical pumping beam so as to generate afundamental wave including multiple linearly polarized modesof a first wavelength and an additional mode of a second
wavelength relatively close to but different from the firstwavelength,
the nonlinear optical material and the lasant material
being positioned between the input mirror and the output mirror
such that (i) the lasant material receives as its input the
optical pumping beam after the pumping beam is caused to passthrough the input mirror, (ii) the nonlinear optical material
receives the fundamental wave generated by the lasant material
as an input, and (iii) the output mirror receives an output fromthe nonlinear optical material,
the nonlinear optical material being configured toproduce as its output an output wave including (i) two
orthogonal linearly polarized modes of the first wavelength,(ii) multiple second harmonic linearly polarized modes of one
half of the first wavelength, and(iii) an additional mode of the second wavelength, andthe laser resonator further including a filter
arrangement for allowing the additional mode and the second
harmonic modes to pass therethrough.
（以下参考：実施の形態（抜粋））5

The operation of the laser in accordance with the present invention will be
described in detail with reference to FIG. 2. As mentioned above, pumping beam 24 isdirected into laser resonator 14 thereby causing lasant material 18 to produce
fundamental wave 26. With the configuration described above, fundamental wave 26 isactually made up of multiple spectral modes of light at wavelengths at and/or about thefirst given wavelength. In the situation where Nd:YVO4 is used as the lasant material,
this first given wavelength is 1064 nm and the multiple spectral modes of light aremodes having about this first given wavelength of 1064 nm. Each of these various
modes propagates along the optical axis of the lasant material and each of the modes islinearly polarized as it emits outside the laser cavity. As mentioned in the background,these multiple modes, which have slightly different wavelengths, tend to strongly
couple to one another causing amplitude fluctuations in the fundamental wave.
In addition to the multiple modes clustered immediately around the first given
wavelength, the inventor has discovered that when using a neodymium doped lasantmaterial as described above, fundamental wave 26 also includes an additional mode ormodes at and/or about a second given wavelength relatively close to but different than
the first given wavelength. This additional mode or modes are produced as an intrinsic
transition of the lasant material. In the case of Nd:YVO4, the first given wavelength(the desired main oscillation wavelength of the fundamental wave) is 1064 nm as
mentioned above. For Nd:YVO4, the inventor has discovered that the additionalmode(s) at the second given wavelength have a wavelength at and/or about 1084 nm. In
the case of Nd:YAG, the first given wavelength is also 1064 nm and the additional modeat the second given wavelength is about 1061 nm. For Nd:YLF, the first givenwavelength (the desired main oscillation wavelength) is 1047 nm and the additionalmode at the second given wavelength is at 1053 nm. As described in the background,because the additional mode(s) at the second given wavelength have a wavelength
relatively close to but different than the modes at the first given wavelength, theadditional mode(s) also may strongly couple with the modes at the first givenwavelength causing additional instability in the fundamental wave.

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