초록 ▼

A method for increasing the efficiency of generating lasers by pumping two separate wavelengths into an erbium-based medium to populate the 4I11/2 state and depopulate the 4I13/2 state. A first excitation wavelength region is located between approximately 955 nm to approximately 1100 nm. The second

A method for increasing the efficiency of generating lasers by pumping two separate wavelengths into an erbium-based medium to populate the 4I11/2 state and depopulate the 4I13/2 state. A first excitation wavelength region is located between approximately 955 nm to approximately 1100 nm. The second excitation wavelength region is located between approximately 1600 nm to approximately 1850 nm. This multi-wavelength pumping scheme may be operated in continuous wave or quasi-continuous wave mode.

대표청구항 ▼

What is claimed is: 1. A method of improving lasing efficiency of an erbium-based medium comprising: a. exposing the medium to a first pump radiation of a first wavelength, such that a first erbium ion is excited from a first state to a second state, b. thereby increasing the population of erbium i

What is claimed is: 1. A method of improving lasing efficiency of an erbium-based medium comprising: a. exposing the medium to a first pump radiation of a first wavelength, such that a first erbium ion is excited from a first state to a second state, b. thereby increasing the population of erbium ions in the second state, creating a population inversion necessary for lasing between the second state as the upper lasing state and a third state as the lower lasing state, said third state being different in energy level than the first state, and c. exposing the medium to a second pump radiation of a second wavelength, such that a second erbium ion is excited from the third state to a fourth state, thereby reducing the population of erbium ions in the third state, reducing a bottleneck created by erbium ions populating the third state, and improving the population inversion necessary for lasing between the second state and the third state, wherein the third state is an 4I13/2lower lasing state and the fourth state is an 4I9/2 metastable state or a Stark level in the 4I11/2 state above said second state, and wherein the lasing efficiency between the second state as the upper lasing state and the third state as the lower lasing state is improved. 2. The method of claim 1, wherein the medium is exposed to the first pump radiation and the second pump radiation generally simultaneously. 3. The method of claim 1, wherein the first state is an 4I15/2 ground state and the second state is an 4I11/2 upper lasing state. 4. The method of claim 1, wherein a. the first pump radiation has a wavelength between approximately 955 nanometers to approximately 1100 nanometers and wherein b. the second pump radiation has a wavelength between approximately 1600 nanometers to approximately 1850 nanometers. 5. The method of claim 1, wherein a. the first pump radiation has a wavelength region located between approximately 959 nanometers to approximately 985 nanometers and wherein b. the second pump radiation has a wavelength region located between approximately 1610 nanometers to approximately 1680 nanometers. 6. The method of claim 1, wherein a. the first pump radiation has a wavelength region located between approximately 959 nanometers to approximately 976 nanometers and wherein b. the second pump radiation has a wavelength region located between approximately 1610 nanometers to approximately 1680 nanometers. 7. The method of claim 1, wherein the first pump radiation and the second pump radiation are continuous waves. 8. The method of claim 1, wherein the first pump radiation and the second pump radiation are pulsed. 9. The method of claim 8, wherein the medium is exposed to the first pump radiation before to exposing the medium to the second pump radiation. 10. The method of claim 9, wherein the exposure to the first pump radiation precedes exposure to the second pump radiation by approximately 100 microseconds. 11. The method of claim 8, wherein the first pump radiation and the second pump radiation are pulsed with a pulse repetition frequency ranging between approximately 1 Hz to approximately 100 kHz.