Bundle of optical fibers for transmission of electromagnetic radiation of high luminous intensity

Claim 2

A flexible fiber bundle comprising a plurality of multimode single fibers having a core and cladding and combined at the ends of the fiber bundle, for high-energy transmission of continuous or pulsed electromagnetic radiation with pulse durations of more than 1 μs and a luminous intensity of from 10 5 W/(rad·mm) 2 to 1.6·10 8 W/(rad·mm) 2 , and for pulsed laser beams having pulse durations of less than 1 μs with a luminous intensity of 10 6 W/(rad·mm) 2 to 8·10 8 W/(rad·mm) 2 , said fiber bundle having: (a) a cross-sectional area A b in mm 2 of (1 . . . 6)·P/I dam , wherein P is the maximum radiant power (pulse peak power) in watts and I dam is the damage threshold value of the fiber bundle in W/mm 2 , and (b) the numerical aperture NA of the fibers in the fiber bundle amounts to the maximum of the quotient of ##EQU6## wherein θ(φ) is the full angular divergence of the beam at the output of the radiation source in rad in dependence on the angle φ perpendicular to the beam axis; D(φ) is the chord and/or diameter of the beam passing through the apex of the angle φ in mm at the output of the radiation source in dependence on the angle φ; D b (φ) is the chord and/or diameter of the beam passing through the apex of the angle φ in mm at the input coupling end of the fiber bundle in dependence on the angle φ, and the numerical aperture is no smaller than 0.05 and no larger than 0.35, and (c) the core diameter of the fibers of the fiber bundle is D k =NA 2 ·b·R, NA meaning the numerical aperture, R meaning the required minimum bending radius in mm, and b meaning a constant having values from 0.03 to 0.24 but being larger than 0.8·λ/NA wherein λ is the wavelength of the radiation to be transmitted in mm, and NA means the numerical aperture of the fibers.

Claim 3

A flexible fiber bundle comprising a plurality of multimode single fibers having a core and cladding and combined at the ends of the fiber bundle, for high-energy transmission of continuous or pulsed electromagnetic radiation with pulse durations of more than 1 μs and a luminous intensity of from 10 5 W/(rad·mm) 2 to 1.6·10 8 W/(rad·mm) 2 , and for pulsed laser beams having pulse durations of less than 1 μs with a luminous intensity of 10 6 W/(rad·mm) 2 to 8·10 8 W/(rad·mm) 2 , said fiber bundle having: (a) a cross-sectional area A b in mm 2 of (1 . . . 6)·P/I dam , wherein P is the maximum radiant power (pulse peak power) in watts and I dam is the damage threshold value of the fiber bundle in W/mm 2 , and (b) the numerical aperture NA of the fibers in the fiber bundle amounts to the maximum of the quotient of ##EQU7## wherein θ(φ) is the full angular divergence of the beam at the output of the radiation source in rad in dependence on the angle φ perpendicular to the beam axis; D(φ) is the chord and/or diameter of the beam passing through the apex of the angle φ in mm at the output of the radiation source in dependence on the angle φ; D b (φ) is the chord and/or diameter of the beam passing through the apex of the angle φ in mm at the input coupling end of the fiber bundle in dependence on the angle φ, and the numerical aperture is no smaller than 0.05 and no larger than 0.35.

Claim 4

A flexible fiber bundle comprising a plurality of multimode single fibers having a core and cladding and combined at the ends of the fiber bundle, for high-energy transmission of continuous or pulsed electromagnetic radiation with pulse durations of more than 1 μs and a luminous intensity of from 10 5 W/(rad·mm) 2 to 1.6·10 8 W/(rad·mm) 2 , and for pulsed laser beams having pulse durations of less than 1 μs with a luminous intensity of 10 6 W/(rad·mm) 2 to 8·10 8 W/(rad·mm) 2 , said fiber bundle having: (a) a cross-sectional area A b in mm 2 of (1 . . . 6)·P/I dam , wherein P is the maximum radiant power (pulse peak power) in watts and I dam is the damage threshold value of the fiber bundle in W/mm 2 , and (b) the numerical aperture NA of the fibers in the fiber bundle amounts to the maximum of the quotient of ##EQU7## wherein θ(φ) is the full angular divergence of the beam at the output of the radiation source in rad in dependence on the angle φ perpendicular to the beam axis; D(φ) is the chord and/or diameter of the beam passing through the apex of the angle φ in mm at the output of the radiation source in dependence on the angle φ; D b (φ) is the chord and/or diameter of the beam passing through the apex of the angle φ in mm at the input coupling end of the fiber bundle in dependence on the angle φ, and the numerical aperture is no smaller than 0.05 and no larger than 0.35.

Claim 5

A fiber bundle according to claim 2 wherein the numerical aperture is between 0.07 and 0.18.

Claim 6

A fiber bundle according to claim 2, wherein the thickness in mm of the cladding of the fibers is larger than 0.05. λ/NA but smaller than 0.05 mm, wherein λ means the wavelength of the radiation to be transmitted in mm, and NA means the numerical aperture of the fibers.

Claim 7

A fiber bundle according to claim 2, wherein the fibers of the fiber bundle are entirely of partially freed of their cladding at the input coupling end and, optionally, at the output coupling end.

Claim 8

A fiber bundle according to claim 2, wherein the fibers are fused together over their entire length.

Claim 9

A fiber bundle according to claim 2, wherein the numerical aperture of the fiber bundle, for rotationally symmetrical beams, is between 0.44·(θ·D)/A b 1/2 and 0.89·(θ·D)/A b 1/2 .

Claim 10

In a process for transmission of high-power, electromagnetic radiation through a flexible fiber bundle comprising a plurality of multimode single fibers having a core and cladding and combined at the ends of the fiber bundle, for continuous or pulsed radiation with pulse durations of more than 1 μs and a luminous intensity of from 10 5 W/(rad·mm) 2 to 1.6·10 8 W/(rad·mm) 2 , and for pulsed laser beams having pulse durations of less than 1 μs with a luminous intensity of 10 6 W/(rad·mm) 2 to 8·10 8 W/(rad·mm) 2 , the improvement comprising passing said radiation through a flexible fiber bundle having: (a) a cross-sectional area A b in mm 2 of (1 . . . 6)·P/I dam , wherein P is the maximum radiant power (pulse peak power) in watts and I dam is the damage threshold value of the fiber bundle in W/mm 2 , (b) the numerical aperture NA of the fibers in the fiber bundle amounts to the maximum of the quotient of ##EQU8## wherein θ(φ) is the full angular divergence of the beam at the output of the radiation source in rad in dependence on the angle φ perpendicular to the beam axis; D(φ) is the chord and/or diameter of the beam passing through the apex of the angle φ in mm at the output of the radiation source in dependence on the angle φ; D b (φ) is the chord and/or diameter of the beam passing through the apex of the angle φ in mm at the input coupling end of the fiber bundle in dependence on the angle φ, and the numerical aperture is no smaller than 0.05 and no larger than 0.35, and (c) the core diameter of the fibers of the fiber bundle is D k =NA 2 ·b·R, NA meaning the numerical aperture, R meaning the required minimum bending radius in mm, and b meaning a constant having values from 0.03 to 0.24 but being larger than 0.8.λ/NA wherein λ is the wavelength of the radiation to be transmitted in mm, and NA means the numerical aperture of the fibers.

Claim 11

In a process for transmission of high-power, electromagnetic radiation through a flexible fiber bundle comprising a plurality of multimode single fibers having a core and cladding and combined at the ends of the fiber bundle, for continuous or pulsed radiation with pulse durations of more than 1 μs and a luminous intensity of from 10 5 W/(rad·mm) 2 to 1.6·10 8 W/(rad·mm) 2 , and for pulsed laser beams having pulse durations of less than 1 μs with a luminous intensity of 10 6 W/(rad·mm) 2 to 8·10 8 W/(rad·mm) 2 , the improvement comprising passing said radiation through a flexible fiber bundle having: (a) a cross-sectional area A b in mm 2 of (1 . . . 6)·P/I dam , wherein P is the maximum radiant power (pulse peak power) in watts and I dam is the damage threshold value of the fiber bundle in W/mm 2 , (b) the numerical aperture NA of the fibers in the fiber bundle amounts to the maximum of the quotient of ##EQU8## wherein θ(φ) is the full angular divergence of the beam at the output of the radiation source in rad in dependence on the angle φ perpendicular to the beam axis; D(φ) is the chord and/or diameter of the beam passing through the apex of the angle φ in mm at the output of the radiation source in dependence on the angle φ; D b (φ) is the chord and/or diameter of the beam passing through the apex of the angle φ in mm at the input coupling end of the fiber bundle in dependence on the angle φ, and the numerical aperture is no smaller than 0.05 and no larger than 0.35, and (c) the core diameter of the fibers of the fiber bundle is D k =NA 2 ·b·R, NA meaning the numerical aperture, R meaning the required minimum bending radius in mm, and b meaning a constant having values from 0.03 to 0.24 but being larger than 0.8.λ/NA wherein λ is the wavelength of the radiation to be transmitted in mm, and NA means the numerical aperture of the fibers.

Claim 12

The process of claim 8, wherein the fiber bundle consists of fibers having essentially the same core diameter.

Claim 13

In a process for transmission of high-power, electromagnetic radiation through a flexible fiber bundle comprising a plurality of multimode single fibers having a core and cladding and combined at the ends of the fiber bundle, for continuous or pulsed radiation with pulse durations of more than 1 μs and a luminous intensity of from 10 5 W/(rad·mm) 2 to 1.6·10 8 W/(rad·mm) 2 , and for pulsed laser beams having pulse durations of less than 1 μs with a luminous intensity of 10 6 W/(rad·mm) 2 to 8·10 8 W/(rad·mm) 2 , the improvement comprising passing said radiation through a flexible fiber bundle having: (a) a cross-sectional area A b in mm 2 of (1 . . . 6)·P/I dam , wherein P is the maximum radiant power (pulse peak power) in watts and I dam is the damage threshold value of the fiber bundle in W/mm 2 , and (b) the numerical aperture NA of the fibers in the fiber bundle amounts to the maximum of the quotient ##EQU9## wherein θ(φ) is the full angular divergence of the beam at the output of the radiation source in rad in dependence on the angle φ perpendicular to the beam axis; D(φ) is the chord and/or diameter of the beam passing through the apex of the angle φ in mm at the output of the radiation source in dependence on the angle φ; D b (φ) is the chord and/or diameter of the beam passing through the apex of the angle φ in mm at the input coupling end of the fiber bundle in dependence on the angle φ, and the numerical aperture is no smaller than 0.05 and no larger than 0.35.

Claim 14

In a process for transmission of high-power, electromagnetic radiation through a flexible fiber bundle comprising a plurality of multimode single fibers having a core and cladding and combined at the ends of the fiber bundle, for continuous or pulsed radiation with pulse durations of more than 1 μs and a luminous intensity of from 10 5 W/(rad·mm) 2 to 1.6·10 8 W/(rad·mm) 2 , and for pulsed laser beams having pulse durations of less than 1 μs with a luminous intensity of 10 6 W/(rad·mm) 2 to 8·10 8 W/(rad·mm) 2 , the improvement comprising passing said radiation through a flexible fiber bundle having: (a) a cross-sectional area A b in mm 2 of (1 . . . 6)·P/I dam , wherein P is the maximum radiant power (pulse peak power) in watts and I dam is the damage threshold value of the fiber bundle in W/mm 2 , and (b) the numerical aperture NA of the fibers in the fiber bundle amounts to the maximum of the quotient ##EQU9## wherein θ(φ) is the full angular divergence of the beam at the output of the radiation source in rad in dependence on the angle φ perpendicular to the beam axis; D(φ) is the chord and/or diameter of the beam passing through the apex of the angle φ in mm at the output of the radiation source in dependence on the angle φ; D b (φ) is the chord and/or diameter of the beam passing through the apex of the angle φ in mm at the input coupling end of the fiber bundle in dependence on the angle φ, and the numerical aperture is no smaller than 0.05 and no larger than 0.35.

Claim 15

The process of claim 10, wherein the numerical aperture is between 0.07 to 0.18.

Claim 16

The process of claim 10, wherein the thickness in mm of the cladding of the fibers is larger than 0.05·λ/NA but smaller than 0.05 mm, wherein λ means the wavelength of the radiation to be transmitted in nm, and NA means the numerical aperture of the fibers.

Claim 17

The process of claim 10, wherein the fibers of the fiber bundle are entirely or partially freed of their cladding at the input coupling end and, optionally, at the output coupling end.

Claim 18

The process of claim 10, wherein the fibers are fused together over their entire length.

Claim 19

The process of claim 10, wherein the numerical aperture of the fiber bundle, for rotationally symmetrical bases, is between 0.44·(θ·D/A b 1/2 and 0.89·(θ·D)A b 1/2 .

Claim 20

The process of claim 10 wherein the fibers lie loosely in the fiber bundle, and the thickness in mm of the fiber cladding is larger than 0.1·λ/NA, wherein NA is the numerical aperture of the fiber and λ is the wavelength of the radiation being transmitted.

Claim 21

The process of claim 14, wherein the cross-sectional area A b of the fiber bundle is smaller than about 4 mm 2 .

Claim 22

The process of claim 10, wherein the fiber bundle is surrounded by a protective sheath.

Claim 23

The process of claim 10 , wherein the fiber bundle is cooled.

Claim 24

The process of claim 10, wherein the cross-sectional profile of the input coupling end of the fiber bundle corresponds to the shape of the beam profile of the electromagnetic radiation being coupled in.

Claim 25

The process of claim 10, wherein the aperture of the beam is modified by redistributing the fibers in the fiber bundle, with the position of the fibers in the input coupling end differing from their respective position in the output coupling end.

Claim 26

The process of claim 21, wherein the fiber bundle contains filler fibers at its output coupling end.

Claim 27

The process of claim 10, wherein several sources of high energy electromagnetic radiation are transmitted together over a multiplexed system by passing the sources of radiation into the input end of a plurality of fiber bundles having their input coupling ends joined into a single bundle.

Claim 28

The process of claim 10, wherein the electromagnetic radiation transmitted in the fiber bundle is divided in a multiplexed system on the output coupling end by subdivision of the fiber bundle into several smaller fiber bundles or fibers.

Claim 29

The process of claim 10, wherein said electromagnetic radiation is transmitted through a bilateral multiplexing system containing at least one of said flexible fiber bundles.

Claim 30

The process of claim 10, wherein the electromagnetic radiation is a laser.