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US 4,233,570 AGranted
Tunable, rare earth-doped solid state lasers
AssigneeThe United States of America as represented by the United States Department of Energy
InventorsJohn L. Emmett, Ralph R. Jacobs, William F. Krupke, Marvin J. Weber
Life of this patent
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Abstract
Laser apparatus comprising combinations of an excimer pump laser and a rare earth-doped solid matrix, utilizing the 5d-4f radiative transition in a rare earth ion to produce visible and ultra-violet laser radiation with high overall efficiency in selected cases and relatively long radiative lifetimes.
Claims7
A method for producing tunable laser light in the visible and ultraviolet, the method comprising the steps of:
- exciting a rare gas-halogen gas or rare gas dimer so that the gas emits radiation at a wavelengths substantially below .lambda.=4500 A;
- directing a portion of the emitted radiation to a solid matrix which is doped by rare earth ion in a fraction 0.1-2.0% numerical density;
- causing a substantial number of rare earth ions in the dopant to be excited into a 5d spectroscopic level of the ions by absorption of the emitted radiation;
- allowing the excited rare earth ions to decay non-radiatively to an energy level substantially at the lower end of the 5d band that has a radiative lifetime exceeding 65 nsec.;
- allowing the excited rare earth ion to decay radiatively from its position substantially at the lower end of the 5d absorption band, with the emission radiation at a wavelength in the wavelength region 1700 A <.lambda.<5200 A.
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A method for producing tunable laser light in the visible and ultraviolet, the method comprising the steps of:
- exciting a rare gas dimer so that the gas emits radiation at wavelengths substantially below .lambda.=4500 A;
- directing a portion of the emitted radiation to a solid matrix which is doped by rare earth ions in a fraction 0.1 to 2.0% numerical density;
- causing a substantial number of rare earth ions in the dopant to be excited into a 5d spectroscopic level of the ions by absorption of the emitted radiation;
- allowing the excited rare earth ions to decay non-radiatively to an energy level substantially at the lower end of the 5d band;
- allowing the excited rare earth ions to decay radiatively from a position substantially at the lower end of the 5d absorption band, with the emission radiation at a wavelength in the wavelength region 1700 A <.lambda.<5200 A.
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Solid state laser apparatus comprising:
- a solid matrix of YAG or NaF, which is substantially transparent to radiation in the wavelength range 2400 A<.lambda.<4000 A;
- a Ce dopant, being present in the solid matrix in a fraction 0.01% to 2% of the numerical density of atoms of the solid matrix, with an ion of the dopant having at least one 5d spectroscopic atomic level lying above the 4f spectroscopic levels of the ion;
- pump means to excite a substantial number of Ce ions into an absorption band that contains said 5d spectroscopic level for the ions.
Solid state laser apparatus comprising:
- a solid matrix that is substantially transparent to radiation in the wavelength range 2400 A <.lambda.<4000 A;
- a rare earth dopant, being present in the solid matrix in a fraction 0.01% to 2% of the numerical density of atoms of the solid matrix, with an ion of the rare earth dopant having at least one 5d spectroscopic atomic level lying above the 4f spectroscopic levels of the ion;
- pump means to excite a substantial number of rare earth ions into an absorption band which contains said 5d spectroscopic level for the ions, with the pump means including a rare gas dimer which, when excited, emits in said wavelength region, the rare gas dimer being selected from the group consisting of Ar.sub.2, Kr.sub.2 and Xe.sub.2.
Solid state laser apparatus comprising:
- a solid matrix that is substantially transparent to radiation in the wavelength range 2400 A <.lambda.<4000 A;
- a rare earth dopant, being present in the solid matrix in a fraction 0.01% to 2% of the numerical density of atoms of the solid matrix, with an ion of the rare earth dopant having at least one 5d spectroscopic atomic level lying substantially above the 4f spectroscopic levels of the ion;
- pump means to excite a substantial number of rare earth ions into an absorption band which contains said 5d spectroscopic level for the ions, with the pump means including the XeF or the N.sub.2 molecule.
Solid state laser apparatus comprising:
- a solid matrix, drawn from the group consisting of CaF.sub.2, BaF.sub.2, SrF.sub.2, SrAl.sub.2 O.sub.4, which is substantially transparent to radiation in the wavelength range 2400 A <.lambda.<4000 A;
- a rare earth dopant, drawn from the divalent group consisting of Eu.sup.2+ and Yb.sup.2+, being present in the solid matrix in a fraction 0.01% to 2% of the numerical density of atoms of the solid matrix, with an ion of the rare earth dopant having at least one 5d spectroscopic atomic level lying substantially above the 4f spectroscopic levels of the ion;
- and
- pump means to excite a substantial number of rare earth ions into an absorption band which contains said 5d spectroscopic level for the ions.
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Dependencies are inferred from the claim text.