Method and apparatus for optimizing the target intensity distribution transmitted from a fiber coupled array
View Patent ↗Encircled far field energy is substantially increased by modifying the near field energy distribution of radiation from each fiber in an emitting array. Each beamlet output from a fiber is modified to have a generally uniform cross-sectional energy distribution, using a pair of aspheric optical elements selected for that purpose. The optical elements may be refractive or reflective. The modified beamlets combine to form a composite output beam with a generally uniform energy distribution. Preferably, the composite beam is subject to an array-wide inverse transformation to a near-Gaussian distribution, further enhancing the encircled far field energy and providing a more efficient high power laser source. Further gains in efficiency are achieved by selecting a fiber bundle pattern, lens array pattern and lens shape that together result in a high fill factor.
1. Apparatus providing increased encircled far field energy in a high power laser, comprising:
an array of optical fibers, each of which emits electromagnetic radiation with a characteristic cross-sectional energy distribution; and
first and second arrays of optical elements aligned to receive radiation from the array of fibers, wherein each optical element in the first array is an aspheric element designed to produce a uniform cross-sectional energy distribution without regard to perfect beam collimation, and wherein each optical element in the second array is an aspheric element designed to collimate radiation transmitted by the corresponding optical element in the first array;
and wherein the combined first and second arrays of optical elements produce an array output of beamlets that form a composite output beam with a generally uniform cross-sectional energy distribution that results in an increased far field encircled energy;
the apparatus further comprising:
first and second array-wide optical elements disposed in the composite output beam to effect an inverse transformation of the composite output beam from a generally uniform energy distribution to a more desirable energy distribution that further increases the far field encircled energy.
2. Apparatus as defined in claim 1 , wherein first and second arrays of optical elements and the first and second array-wide optical elements are selected from refractive optical elements and reflective optical elements.
3. Apparatus as defined in claim 1 , wherein the optical elements in the first and second arrays are aspheric lenses.
4. Apparatus as defined in claim 1 , wherein the optical elements in the first and second arrays are aspheric mirrors.
5. Apparatus as defined in claim 1 , wherein:
the array of fibers has individual fibers centered on a square pattern;
the first and second arrays have their optical elements centered on a square pattern to receive radiation from the fibers; and
the optical elements in the first and second arrays are square in cross-sectional shape to provide a large fill factor that also contributes to an increase in the far field encircled energy.
6. Apparatus as defined in claim 1 , wherein:
the array of fibers has individual fibers centered on a hexagonal pattern;
the first and second arrays have their optical elements centered on a hexagonal pattern to receive radiation from the fibers; and
the optical elements in the first and second arrays are hexagonal in cross-sectional shape to provide a large fill factor that also contributes to an increase in the far field encircled energy.
7. Apparatus as defined in claim 1 , wherein:
the array of fibers has individual fibers centered on a square pattern;
the first and second arrays have their optical elements centered on a square pattern to receive radiation from the fibers; and
the optical elements in the first and second arrays, and the first and second array-wide optical elements, are square in cross-sectional shape to provide a large fill factor that also contributes to an increase in the far field encircled energy.
8. Apparatus as defined in claim 1 , wherein:
the array of fibers has individual fibers centered on a hexagonal pattern;
the first and second arrays have their optical elements centered on a hexagonal pattern to receive radiation from the fibers; and
the optical elements in the first and second arrays, and the first and second array-wide optical elements, are hexagonal in cross-sectional shape to provide a large fill factor that also contributes to an increase in the far field encircled energy.
9. A method for providing increased encircled far field energy in a high power laser, comprising:
emitting electromagnetic radiation from each element of an array of optical fibers, wherein each of the fibers emits radiation with a characteristic cross-sectional energy distribution;
aligning first and second arrays of optical elements to receive radiation from the array of fibers, wherein each optical element in the first array is an aspheric element designed to produce a uniform cross-sectional energy distribution without regard to perfect beam collimation, and wherein each optical element in the second array is an aspheric element designed to collimate radiation transmitted by the corresponding optical element in the first array; and
producing in the combined first and second arrays of optical elements an array of output beamlets that together form a composite output beam with a generally uniform cross-sectional energy distribution that results in an increased far field encircled energy;
the method further comprising:
disposing first and second array-wide optical elements in the composite output beam to effect an inverse transformation of the composite output beam from a generally uniform energy distribution to a more desirable energy distribution that further increases the far field encircled energy.
10. A method as defined in claim 9 , wherein the more desirable energy distribution is a Gaussian distribution.
11. A method as defined in claim 9 , wherein first and second arrays of optical elements and the first and second array-wide optical elements are selected from refractive optical elements and reflective optical elements.
12. A method as defined in claim 9 , wherein the optical elements in the first and second arrays are aspheric lenses.
13. A method as defined in claim 9 , wherein the optical elements in the first and second arrays are aspheric mirrors.
14. A method as defined in claim 9 , and further comprising:
centering individual fibers in the array of fibers on a square matrix pattern; and centering individual optical elements of the first and second arrays on a square matrix pattern to receive radiation from the fibers;
wherein the optical elements in the first and second arrays are square in cross-sectional shape to provide a large fill factor that also contributes to an increase in the far field encircled energy.
15. A method as defined in claim 9 , and further comprising:
centering individual fibers in the array of fibers on a hexagonal matrix pattern; and
centering individual optical elements in the first and second arrays on a hexagonal matrix pattern to receive radiation from the fibers;
wherein the optical elements in the first and second arrays are hexagonal in cross-sectional shape to provide a large fill factor that also contributes to an increase in the far field encircled energy.
16. A method as defined in claim 9 , and further comprising:
centering individual fibers in the array of fibers on a square matrix pattern; and
centering individual optical elements of the first and second arrays on a square matrix pattern to receive radiation from the fibers;
wherein the optical elements in the first and second arrays, and the first and second array-wide optical elements, are square in cross-sectional shape to provide a large fill factor that also contributes to an increase in the far field encircled energy.
17. A method as defined in claim 9 , and further comprising:
centering individual fibers in the array of fibers on a hexagonal matrix pattern; and
centering individual optical elements in the first and second arrays on a hexagonal matrix pattern to receive radiation from the fibers;
wherein the optical elements in the first and second arrays, and the first and second array-wide optical elements, are hexagonal in cross-sectional shape to provide a large fill factor that also contributes to an increase in the far field encircled energy.
18. A method for providing increased encircled far field energy in a high power laser, comprising:
emitting electromagnetic radiation from each element of an array of optical fibers, wherein each of the fibers emits radiation with a characteristic cross-sectional energy distribution;
aligning first and second arrays of optical elements to receive radiation from the array of fibers, wherein each optical element in the first array is an aspheric element designed to produce a uniform cross-sectional energy distribution without regard to perfect beam collimation, and wherein each optical element in the second array is an aspheric element designed to collimate radiation transmitted by the corresponding optical element in the first array; and
producing in the combined first and second arrays of optical elements an array of output beamlets that together form a composite output beam with a generally uniform cross-sectional energy distribution that results in an increased far field encircled energy;
the method further comprising:
adjusting output intensities of individual elements of the array of optical fibers, to modify the generally uniform cross-sectional energy distribution of the composite output beam to a more desirable energy distribution that further increases the far field encircled energy.
19. A method for providing desired distributions of amplitude and phase structure in a high power laser, comprising:
emitting electromagnetic radiation from each element of an array of optical fibers, wherein each of the fibers emits radiation with a characteristic cross-sectional energy distribution;
aligning first and second arrays of optical elements to receive radiation from the array of fibers, wherein each optical element in the first array is an aspheric element designed to produce a uniform cross-sectional energy distribution without regard to perfect beam collimation, and wherein each optical element in the second array is an aspheric element designed to collimate radiation transmitted by the corresponding optical element in the first array;
producing in the combined first and second arrays of optical elements an array of output beamlets that together form a composite output beam with a generally uniform cross-sectional energy distribution that results in an increased far field encircled energy; and
disposing first and second array-wide optical elements in the composite output beam to effect a further transformation of the composite output beam from a generally uniform energy distribution to a more desirable energy distribution that has the desired amplitude and phase structure in the near field and produces an optimum energy distribution at a desired range from the array.
20. A method as defined in claim 19 , wherein the more desirable energy distribution is a Bessel distribution.