LOW-NOISED FULL SOLID STATE SECOND HARMONIC LASER GENERATOR

PROBLEM TO BE SOLVED: To reduce the noise by setting the position at least near the center of a solid state laser crystal where the light intensity is substantially zero in the longitudinal multi-mode of a fundamental wave in a resonator. SOLUTION: The position (z) of a solid state laser crystal 4 f...

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Main Authors MITA MASAHIRO, MAKIO SATOSHI, ISHIDA HIDENOBU
Format Patent
LanguageEnglish
Published 21.04.2000
Edition7
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Abstract PROBLEM TO BE SOLVED: To reduce the noise by setting the position at least near the center of a solid state laser crystal where the light intensity is substantially zero in the longitudinal multi-mode of a fundamental wave in a resonator. SOLUTION: The position (z) of a solid state laser crystal 4 from a first laser mirror 3 in a resonator is set and length of the resonator is given Lc, so that z=Lc.n/(m.q), n≠j.m (n, m, q and j are each a positive integer, (m) is the longitudinal mode number generated in the resonator, and (q) is the interval of the longitudinal mode). Since no space hold burning occurs at the position (z) in the equation, no mode competition occurs to result in a low noise with the laser crystal 4 set at the position (z). When the focal point position (w) of an exciting light is the same as the position (z) in the equation, the exciting energy concentrates to bring out a more high effect.
AbstractList PROBLEM TO BE SOLVED: To reduce the noise by setting the position at least near the center of a solid state laser crystal where the light intensity is substantially zero in the longitudinal multi-mode of a fundamental wave in a resonator. SOLUTION: The position (z) of a solid state laser crystal 4 from a first laser mirror 3 in a resonator is set and length of the resonator is given Lc, so that z=Lc.n/(m.q), n≠j.m (n, m, q and j are each a positive integer, (m) is the longitudinal mode number generated in the resonator, and (q) is the interval of the longitudinal mode). Since no space hold burning occurs at the position (z) in the equation, no mode competition occurs to result in a low noise with the laser crystal 4 set at the position (z). When the focal point position (w) of an exciting light is the same as the position (z) in the equation, the exciting energy concentrates to bring out a more high effect.
Author MITA MASAHIRO
MAKIO SATOSHI
ISHIDA HIDENOBU
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Snippet PROBLEM TO BE SOLVED: To reduce the noise by setting the position at least near the center of a solid state laser crystal where the light intensity is...
SourceID epo
SourceType Open Access Repository
SubjectTerms BASIC ELECTRIC ELEMENTS
DEVICES OR ARRANGEMENTS, THE OPTICAL OPERATION OF WHICH ISMODIFIED BY CHANGING THE OPTICAL PROPERTIES OF THE MEDIUM OF THEDEVICES OR ARRANGEMENTS FOR THE CONTROL OF THE INTENSITY,COLOUR, PHASE, POLARISATION OR DIRECTION OF LIGHT, e.g.SWITCHING, GATING, MODULATING OR DEMODULATING
DEVICES USING STIMULATED EMISSION
ELECTRICITY
FREQUENCY-CHANGING
NON-LINEAR OPTICS
OPTICAL ANALOGUE/DIGITAL CONVERTERS
OPTICAL LOGIC ELEMENTS
OPTICS
PHYSICS
TECHNIQUES OR PROCEDURES FOR THE OPERATION THEREOF
Title LOW-NOISED FULL SOLID STATE SECOND HARMONIC LASER GENERATOR
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