Method of forming an avalanche semiconductor photo-detector device and a device thus formed

Claim 1

A process for forming an avalanche photodetector of the type comprising at least one photon absorption region in which carriers are photoinduced, made from a first semiconductor material with narrow prohibited band width, a carrier multiplication region made from a second semiconductor material with wide prohibited band width, and a third intermediate region formed by a lattice of slices of alternating layers of the first and second materials forming a system of coupled quantum wells separated by potential barriers, wherein, with the photodetector and operating conditions therefor being specified comprising a given band discontinuity and local electric field as well as a maximum response time, comprising a sequence of steps for determining said intermediate region comprising a minimum number of slices of alternating layers of varying thicknesses ensuring a response time less than or equal to said maximum response time, said sequence of steps comprising: (a) determining the respective thicknesses of the layers made from the first and second semiconductor materials forming said slices of the intermediate region of a system comprising a single quantum well ensuring a minimum intermediate response time of said system; (b) comparing this minimum intermediate response time with said maximum response time; and (c) conditionally repeating steps (a) and (b) by progressively increasing the number of coupled wells until the response time obtained for a system comprising a given number of coupled quantum wells is less than said maximum response time or until the response time for this system comprising said given number of coupled quantum wells is greater than or equal to the response time for a system comprising a number of coupled wells one less than said given number.

Claim 3

A method of forming an avalanche photodetector of the type comprising at least one photon absorption region in which carriers are photoinduced, made from a first semiconductor material with narrow prohibited band width, a carrier multiplication region made from a second semiconductor material with wide prohibited band width, and a third intermediate region formed by a lattice of slices of given layers of the first and second materials forming a system of coupled quantum wells separated by potential barriers; wherein, with the photodetector and operating conditions therefor being specified comprising band discontinuity and a given local electric field as well as a maximum response time, including a determination for said intermediate region comprising a minimum number of slices of alternating layers of varying thicknesses ensuring a response time less than or equal to said maximum response time, said determination comprising: (a) determining the thickness of the first layer made from the first material forming a well so that the time for evacuating a carrier trapped in this well to the material of wide prohibited band width is less than half said maximum response time; (b) determining the thicknesses of the slices which follow, made respectively from the second material forming a barrier and from the first material forming a well, so that the escape time to the preceding well is less than or equal to a given fraction of the maximum response time, and so that the new well is the thickest possible; (c) conditionally repeating step (b) while progressively increasing the number of coupled quantum wells so as to form a structure of coupled quantum wells of increasing thicknesses, said repetition taking place until a determined width of the last well tends towards infinity or until said determined width is not strictly greater than that of the well which precedes it.

Claim 4

A method of forming an avalanche photodetector of the type comprising at least one photon absorption region in which carriers are photoinduced, made from a first semiconductor material with narrow prohibited band width, a carrier multiplication region made from a second semiconductor material with wide prohibited band width, and a third intermediate region formed by a lattice of slices of given layers of the first and second materials forming a system of coupled quantum wells separated by potential barriers; wherein, with the photodetector and operating conditions therefor being specified comprising band discontinuity and a given local electric field as well as a maximum response time, including a determination for said intermediate region comprising a minimum number of slices of alternating layers of varying thicknesses ensuring a response time less than or equal to said maximum response time, said determination comprising: (a) determining the thickness of the first layer made from the first material forming a well so that the time for evacuating a carrier trapped in this well to the material of wide prohibited band width is less than half said maximum response time; (b) determining the thicknesses of the slices which follow, made respectively from the second material forming a barrier and from the first material forming a well, so that the escape time to the preceding well is less than or equal to a given fraction of the maximum response time, and so that the new well is the thickest possible; (c) conditionally repeating step (b) while progressively increasing the number of coupled quantum wells so as to form a structure of coupled quantum wells of increasing thicknesses, said repetition taking place until a determined width of the last well tends towards infinity or until said determined width is not strictly greater than that of the well which precedes it.