Non-reflective/reflective phase transition optical modulator
AssigneeNone recorded
InventorJohn C. Wert, III
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AssigneeNone recorded
InventorJohn C. Wert, III
Estimating the term…
An optical modulator particularly suited for use as an output coupler from the resonating cavity of a laser. The modulator is fabricated with a semiconducting oxide compound selected from the group consisting of VO, VO.sub.2, V.sub.2 O.sub.3, V.sub.3 O.sub.5, V.sub.4 O.sub.6, V.sub.5 O.sub.9, V.sub.6 O.sub.11, V.sub.7 O.sub.13, V.sub.8 O.sub.15, Ti.sub.2 O.sub.3, Ti.sub.4 O.sub.7, NbO.sub.2, FeSi.sub.2, VO.sub.2 NbO.sub.2, V.sub.1-x Mo.sub.x O.sub.2, VO.sub.2 -TiO.sub.2, V.sub.2 O.sub.3 -Ti.sub.2 O.sub.3, V.sub.1-x Ge.sub.x O.sub.2, V.sub.1-x Nb.sub.x O.sub.2, V.sub.1-x Cr.sub.x O.sub.2, (Cr.sub.x V.sub.1-x).sub.2 O.sub.3 and V.sub.1-x Ti.sub.x O.sub.2. When an electric field is applied to an output coupler fabricated with a thin film or single crystal of material from the foregoing group, the material undergoes a transition between metallic and semiconducting states. In the metallic state the output coupler reflects incident luminous energy. In the semiconducting state, on the other hand, the material transmits such luminous energy. Thereby, a laser system output coupler fabricated with a material from the above-defined group can, by external stimulation, be caused to reflect back or transmit out the laser energy stored within the resonating cavity. Furthermore, since transition between states can be performed with speeds ranging from microseconds to nanoseconds, the output coupler is compatible with the needs of Q-switched or cavity dumped laser configurations.
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An output coupler for the resonating cavity of a repetitively pulsed laser, comprising:
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From the US filing history. Foreign family members aren’t listed.
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1. Field of the Invention
The invention disclosed herein relates to modulators of luminous energy typified by that generated in lasers, and particularly those modulators fabricated with oxide compounds which undergo transitions between metallic and non-metallic states in response to external stimuli.
2. Description of the Prior Art
FIGS. 1a and 1b schematically show the respective layouts of a conventional Q-switched laser and a conventional cavity dumped laser.
FIG. 2a schematically depicts a single crystal structure fabricated from one of the oxide compounds in the group.
FIG. 2b is a schematic of another embodiment, wherein a thin film of the compound is sandwiched between transparent materials.
FIGS. 1a and 1b schematically represent two of the many conventional laser configurations, these two being known in the parlance of the art as a Q-switched laser and a cavity dumped laser, respectively. In the Q-switched laser of FIG. 1a rotating mirror 1 is synchronized with the transmission of luminous energy 3 from flash lamp type pump 2 into gain medium 4 of the laser's resonating cavity. When mirror 1 rotates into alignment, lasing commences. Output coupling mirror 6 normally transmits about 30% of the incident luminous energy, reflecting the remainder back into gain medium 4. Thereby, laser output 7 consists of pulses having a repetition rate corresponding to the rotation rate of mirror 1.
The cavity dumped configuration in FIG. 1b extracts a laser pulse by deflecting the luminous energy beam. As with the Q-switched configuration pump 2 supplies luminous energy 3 to gain medium 4 of the laser resonating cavity. At one end of gain medium 4 is stationary mirror 8, while the luminous path from the other end of gain medium 4 communicates with mirror 9, acousto-optic modulator 11, mirror 12, and at times prism 13. Since the configuration in FIG. 1b is well known, it need only be noted that stimulation of acousto-optic modulator 11 alters the path of incident luminous energy onto the path defined by reference line 16. Without stimulation, luminous energy passing through acousto-optic modulator 11 follows the path defined by dashed line 14, effectively being retroreflective as to gain medium 4.
The central feature of the invention is a utilization of oxide compounds from a defined group to directly control the luminous energy leaving the resonating cavity of a laser. When stimulated, compounds from this group respond by undergoing a transition between metallic and non-metallic states, which correspond to reflection or transmission of the incident luminous energy.