Modified involute flashlamp reflector

Claim 2

A reflector for a laser having a substantially cylindrical flashlamp whose marginal angle, φ m , is less than 90°, said laser reflector comprising a surface of light-reflective material and a cross-section, in a plane perpendicular to the axis of said cylindrical lamp, defined by x=±(r cos θ+rθ sin φ.sub.m (cos φ.sub.m cos θ-sin φ.sub.m sin θ)), and y=r sin θ+rθ sin φ.sub.m (cos φ.sub.m sin θ-sin φ.sub.m cos θ), where x and y are orthogonal axes of a Cartesian coordinate system which axes intersect at the axis of said flashlamp, where θ represents a varying angle of rotation around said flashlamp axis such that 0≦θ<π, and where r is the radius of said cylindrical flashlamp.

Claim 3

A laser including: at least one substantially cylindrical flashlamp including a gas discharge region surrounded by a light-transparent envelope; a coolant material surrounding said flashlamp; a light-transparent laser window in contact with part of said coolant material; and a flashlamp reflector connected to said laser window in fluid-tight relationship, said reflector having a light-reflective surface in contact with said coolant material, said coolant filling substantially the entire volume surrounding said flashlamp and enclosed by said reflector and said window, and said reflector having a reflective surface whose cross section in a plane perpendicular to said flashlamp axis is defined by x=±(r.sub.o cos θ+r.sub.o θ sin φ.sub.m (cos φ.sub.m cos θ-sin φ.sub.m sin θ)), y=r.sub.o sin θ+r.sub.o θ sin φ.sub.m (cos φ.sub.m sin θ-sin φ.sub.m cos θ), where x and y represent orthogonal axes in a Cartesian coordinate system which axes intersect at said flashlamp axis, where θ represents a varying angle of rotation around said flashlamp axis between zero and pi radius where r o is the outer diameter of said transparent flashlamp envelope, and where φ m is a marginal angle defined by the equation φ.sub.m =sin.sup.-1 (n.sub.e /n.sub.c sin φ'), where n e is refractive index of said flash lamp envelope, n c is refractive index of said coolant material, and θ' is defined by the equation ##EQU1## where n p is the refractive index of said gas discharge region, r i is the inside diameter of said flashlamp envelope, ##EQU2##

Claim 4

A laser including: at least one substantially cylindrical flashlamp including a gas discharge region surrounded by a light-transparent envelope; a coolant material surrounding said flashlamp; a light-transparent laser window in contact with part of said coolant material; and a flashlamp reflector connected to said laser window in fluid-tight relationship, said reflector having a light-reflective surface in contact with said coolant material, said coolant filling substantially the entire volume surrounding said flashlamp and enclosed by said reflector and said window, and said reflector having a reflective surface whose cross section in a plane perpendicular to said flashlamp axis is defined by x=±(r.sub.o cos θ+r.sub.o θ sin φ.sub.m (cos φ.sub.m cos θ-sin φ.sub.m sin θ)), y=r.sub.o sin θ+r.sub.o θ sin φ.sub.m (cos φ.sub.m sin θ-sin φ.sub.m cos θ), where x and y represent orthogonal axes in a Cartesian coordinate system which axes intersect at said flashlamp axis, where θ represents a varying angle of rotation around said flashlamp axis between zero and pi radius where r o is the outer diameter of said transparent flashlamp envelope, and where φ m is a marginal angle defined by the equation φ.sub.m =sin.sup.-1 (n.sub.e /n.sub.c sin φ'), where n e is refractive index of said flash lamp envelope, n c is refractive index of said coolant material, and θ' is defined by the equation ##EQU1## where n p is the refractive index of said gas discharge region, r i is the inside diameter of said flashlamp envelope, ##EQU2##

Claim 5

A laser including: two parallel flashlamps having circular cross sections, each including a gas discharge region surrounded by a transparent envelope, the flashlamps having a marginal angle, φ m , less than π/2 radius; a coolant material surrounding each of said flashlamps; two laser windows, each said laser window contacting the coolant material surrounding a different one of said flashlamps; and two flashlamp reflectors each connected to a different one of said laser windows in fluid-tight relationship to bound said coolant material around a different one of said flashlamps, said coolant material filling substantially the entire volume surrounding each said flashlamp, each said reflector having a reflective surface whose cross section in a plane perpendicular to said flashlamps' axes is defined by the equation x=±(r cos θ+rθ sin φ.sub.m (cos φ.sub.m cos θ+sin φ.sub.m sin θ)), and y=r sin θ+rθ sin φ.sub.m (cos φ.sub.m sin θ-sin φ.sub.m cos θ), where x and y are orthogonal axes of a Cartesian coordinate system which intersect at the center of said circular cross section of its corresponding flashlamp, r is the radius of said corresponding flashlamp, and θ is a varying angle of rotation around said flashlamp axis between zero and pi radius.

Claim 6

A laser including: two parallel flashlamps having circular cross sections, each including a gas discharge region surrounded by a transparent envelope, the flashlamps having a marginal angle, φ m , less than π/2 radius; a coolant material surrounding each of said flashlamps; two laser windows, each said laser window contacting the coolant material surrounding a different one of said flashlamps; and two flashlamp reflectors each connected to a different one of said laser windows in fluid-tight relationship to bound said coolant material around a different one of said flashlamps, said coolant material filling substantially the entire volume surrounding each said flashlamp, each said reflector having a reflective surface whose cross section in a plane perpendicular to said flashlamps' axes is defined by the equation x=±(r cos θ+rθ sin φ.sub.m (cos φ.sub.m cos θ+sin φ.sub.m sin θ)), and y=r sin θ+rθ sin φ.sub.m (cos φ.sub.m sin θ-sin φ.sub.m cos θ), where x and y are orthogonal axes of a Cartesian coordinate system which intersect at the center of said circular cross section of its corresponding flashlamp, r is the radius of said corresponding flashlamp, and θ is a varying angle of rotation around said flashlamp axis between zero and pi radius.

Claim 7

A laser including: (a) a plurality of serially-arranged laser sections each including two parallel flashlamps having circular cross sections, each including a gas discharge region surrounded by a transparent envelope, the flashlamps having a marginal angle, φ m , less than 90 degrees, and two flashlamp reflectors each surrounding a different flashlamp and each having a reflective surface whose cross section in a plane perpendicular to said flashlamps' axes is defined by the equation x=±(r cos θ+rθ sin φ.sub.m (cos φ.sub.m cos θ+sin φ.sub.m sin θ)), and y=r sin θ+rθ sin φ.sub.m (cos φ.sub.m sin θ-sin φ.sub.m cos θ), where x and y are orthogonal axes of a Cartesian coordinate system which intersect at the center of said circular cross sections of the flashlamp surrounded by said reflector, r is the radius of said surrounded flashlamp, and θ is a varying angle of rotation around said flashlamp axis between zero and pi radius; (b) two parallel laser windows connected to each of said laser sections so as to form a fluid-tight compartment with each reflector in each laser section, each fluid-tight compartment containing one of said flashlamps; and (c) coolant material surrounding said flashlamps in each of said compartments.

Claim 8

A laser including: (a) a plurality of serially-arranged laser sections each including two parallel flashlamps having circular cross sections, each including a gas discharge region surrounded by a transparent envelope, the flashlamps having a marginal angle, φ m , less than 90 degrees, and two flashlamp reflectors each surrounding a different flashlamp and each having a reflective surface whose cross section in a plane perpendicular to said flashlamps' axes is defined by the equation x=±(r cos θ+rθ sin φ.sub.m (cos φ.sub.m cos θ+sin φ.sub.m sin θ)), and y=r sin θ+rθ sin φ.sub.m (cos φ.sub.m sin θ-sin φ.sub.m cos θ), where x and y are orthogonal axes of a Cartesian coordinate system which intersect at the center of said circular cross sections of the flashlamp surrounded by said reflector, r is the radius of said surrounded flashlamp, and θ is a varying angle of rotation around said flashlamp axis between zero and pi radius; (b) two parallel laser windows connected to each of said laser sections so as to form a fluid-tight compartment with each reflector in each laser section, each fluid-tight compartment containing one of said flashlamps; and (c) coolant material surrounding said flashlamps in each of said compartments.