Abstract: An IGBT includes a mesa section that extends between two cell trench structures from a first surface of a semiconductor portion to a layer section of the semiconductor portion. A source region, which is electrically connected to an emitter electrode, is formed in the mesa section. A doped region, which is separated from the source region by a body region of a complementary conductivity type, includes a first portion with a first mean net impurity concentration and a second portion with a second mean net impurity concentration exceeding at least ten times the first mean net impurity concentration. In the mesa section the first portion extends from the body region to the layer section. The second portions of the doped region virtually narrow the mesa sections in a normal on-state of the IGBT.

Abstract: A semiconductor includes a drift zone of a first conductivity type arranged between a first side and a second side of a semiconductor body. The semiconductor device further includes a first region of the first conductivity type and a second region of a second conductivity type subsequently arranged along a first direction parallel to the second side. The semiconductor device further includes an electrode at the second side adjoining the first and second regions. The semiconductor device further includes a third region of the second conductivity type arranged between the drift zone and the first region. The third region is spaced apart from the second region and from the second side.

Abstract: An IGBT includes a mesa section that extends between two cell trench structures from a first surface of a semiconductor portion to a layer section of the semiconductor portion. A source region, which is electrically connected to an emitter electrode, is formed in the mesa section. A doped region, which is separated from the source region by a body region of a complementary conductivity type, includes a first portion with a first mean net impurity concentration and a second portion with a second mean net impurity concentration exceeding at least ten times the first mean net impurity concentration. In the mesa section the first portion extends from the body region to the layer section. The second portions of the doped region virtually narrow the mesa sections in a normal on-state of the IGBT.

Abstract: A semiconductor includes a drift zone of a first conductivity type arranged between a first side and a second side of a semiconductor body. The semiconductor device further includes a first region of the first conductivity type and a second region of a second conductivity type subsequently arranged along a first direction parallel to the second side. The semiconductor device further includes an electrode at the second side adjoining the first and second regions. The semiconductor device further includes a third region of the second conductivity type arranged between the drift zone and the first region. The third region is spaced apart from the second region and from the second side.

Abstract: The present invention relates to a method for determining an edge profile of a volume of a photoresist after a development process. At first, the volume of the photoresist is divided into cells. A chemical master equation is set up which reflects the stochastic kinetics of chemical reactions proceeding in cells of the volume of the photoresist during the development process. The chemical master equation is solved for a given development time on the basis of a Gillespie algorithm in order to determine developed and non-developed cells of the volume of the photoresist at the end of the development process. Finally, the edge profile of the volume of the photoresist after the development process is determined on the basis of a cluster of non-developed cells.

Abstract: The present invention relates to a method for determining an edge profile of a volume of a photoresist after a development process. At first, the volume of the photoresist is divided into cells. A chemical master equation is set up which reflects the stochastic kinetics of chemical reactions proceeding in cells of the volume of the photoresist during the development process. The chemical master equation is solved for a given development time on the basis of a Gillespie algorithm in order to determine developed and non-developed cells of the volume of the photoresist at the end of the development process. Finally, the edge profile of the volume of the photoresist after the development process is determined on the basis of a cluster of non-developed cells.