GB1073179A - A laser - Google Patents
A laserInfo
- Publication number
- GB1073179A GB1073179A GB4368564A GB4368564A GB1073179A GB 1073179 A GB1073179 A GB 1073179A GB 4368564 A GB4368564 A GB 4368564A GB 4368564 A GB4368564 A GB 4368564A GB 1073179 A GB1073179 A GB 1073179A
- Authority
- GB
- United Kingdom
- Prior art keywords
- microwave
- cavity
- laser
- ruby
- crystal
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/10—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
- H01S3/106—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling devices placed within the cavity
- H01S3/107—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling devices placed within the cavity using electro-optic devices, e.g. exhibiting Pockels or Kerr effect
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/09—Processes or apparatus for excitation, e.g. pumping
- H01S3/091—Processes or apparatus for excitation, e.g. pumping using optical pumping
- H01S3/0915—Processes or apparatus for excitation, e.g. pumping using optical pumping by incoherent light
- H01S3/092—Processes or apparatus for excitation, e.g. pumping using optical pumping by incoherent light of flash lamp
Abstract
1,073,179. Lasers. INTERNATIONAL BUSINESS MACHINES CORPORATION. Oct. 27, 1964 [Oct. 31, 1963], No. 43685/64. Heading H1C. A laser is pulse-frequency modulated by means of an electro-optic crystal included within the laser cavity. As shown in Fig. 2, a laser comprises a ruby crystal 22 surrounded by a pulsed helical flash lamp 24 which may have conventional reflecting and cooling accessories. A beam of stimulated radiation 25 may pass through a polarizing prism 28 having a vertical transmission plane: alternatively, if a 90 degree or 60 degree oriented ruby is used, the polarizing prism is unnecessary. Lenses 30, 32 reduce the plane-polarized beam which passes into a cylindrical waveguide cavity 34 containing centrally an electro-optic crystal 38 having a linear electro-optic effect and a high electrooptic coefficient such as NH 4 H 2 PO 4 , KH 2 PO 4 or KD 2 PO 4 . A generator 18 generates a frequency-modulated microwave signal bearing information which signal is applied to a probe 35 to excite the cavity 34 in its TM 01 mode. The cavity 34 has an axial length equal to an integral number of half-wavelengths of the microwave carrier and a low-loss dielectric 36 such as fused quartz is used to match the phase velocity of the standing microwaves with that of the stimulated radiation. The spacing of the Fabry-Perot reflectors 40, 42 is such that the time for propagation of radiatoin between them is equal to an integral number of half-periods of the microwave carrier. The state of polarization of stimulated radiation re-entering the ruby crystal after reflection from the reflector 42 is modulated by the microwave field within the cavity 34. In Fig. 3 (not shown) laser pulses 50 are emitted from partially reflecting surface 40 twice per microwave cycle when the microwave field is substantially zero. There is described with reference to Figs. 4 and 5 (not shown) an embodiment in which a birefringent bias plate (52) is inserted in the beam between the ruby crystal and the modulator; only one fourth as much modulator power is required but laser pulses are emitted only once per microwave cycle.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US32043963A | 1963-10-31 | 1963-10-31 |
Publications (1)
Publication Number | Publication Date |
---|---|
GB1073179A true GB1073179A (en) | 1967-06-21 |
Family
ID=23246436
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB4368564A Expired GB1073179A (en) | 1963-10-31 | 1964-10-27 | A laser |
Country Status (2)
Country | Link |
---|---|
CH (1) | CH428970A (en) |
GB (1) | GB1073179A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1981002224A1 (en) * | 1980-01-21 | 1981-08-06 | Australia Dept Ind Comm | Birefringence coupled high average power laser |
-
1964
- 1964-10-27 GB GB4368564A patent/GB1073179A/en not_active Expired
- 1964-10-27 CH CH1388964A patent/CH428970A/en unknown
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1981002224A1 (en) * | 1980-01-21 | 1981-08-06 | Australia Dept Ind Comm | Birefringence coupled high average power laser |
Also Published As
Publication number | Publication date |
---|---|
CH428970A (en) | 1967-01-31 |
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