Abstract: A method is disclosed for improving an optical imaging property, for example spherical aberration or the focal length, of a projection objective of a microlithographic projection exposure apparatus. First, an immersion liquid is introduced into an interspace between a photosensitive surface and an end face of the projection objective. Then an imaging property of the projection objective is determined, for example using an interferometer or a CCD sensor arranged in an image plane of the projection objective. This imaging property is compared with a target imaging property. Finally, the temperature of the immersion liquid is changed until the determined imaging property is as close as possible to the target imaging property.

Abstract: A method of adjusting a projection objective permits the projection objective to be adjusted between an immersion configuration and a dry configuration. The projection objective includes optical elements arranged along an optical axis thereof, which include a first group of elements following the object plane and a last optical element following the first group, which is arranged near the image plane. The last optical element defines an exit surface of the projection objective, which is arranged at a working distance from the image plane. The last optical element is substantially without refracting power and has no or only slight curvature. The method includes varying the thickness of the last optical element, changing the refractive index of the space between the exit surface and the image plane by introducing or removing an immersion medium, and axially displacing the last optical element to set a working distance.

Abstract: In a method for manufacturing an optical imaging system, wavefront aberrations caused by an optical imaging system are determined before and after transporting the optical imaging system. At least some of the aberration parameters which are determined in the preceding determination are used as a given precondition for determining aberration parameters in the subsequent determination. This results in a hybrid method, in which the strength of at least two measurement methods are used in a combined form, and specific weaknesses of any one method are avoided.

Abstract: In a method for manufacturing an optical imaging system, wavefront aberrations caused by an optical imaging system are determined before and after transporting the optical imaging system. At least some of the aberration parameters which are determined in the preceding determination are used as a given precondition for determining aberration parameters in the subsequent determination. This results in a hybrid method, in which the strength of at least two measurement methods are used in a combined form, and specific weaknesses of any one method are avoided.

Abstract: In a method for determining wavefront aberrations for the characterization of imaging characteristics in an optical imaging system, the measurement results from two different measurement methods, which are carried out at successive times, are combined. In this case, at least some of the aberration parameters which are determined in the previous first measurement method are used as a given precondition for determining aberration parameters with the aid of the second measurement method, and are assessed accordingly. This results in a hybrid method, in which the strength of at least two measurement methods are used in a combined form, and specific weaknesses of any one method can be avoided.

Abstract: A method is disclosed for improving an optical imaging property, for example spherical aberration or the focal length, of a projection objective of a microlithographic projection exposure apparatus. First, an immersion liquid is introduced into an interspace between a photosensitive surface and an end face of the projection objective. Then an imaging property of the projection objective is determined, for example using an interferometer or a CCD sensor arranged in an image plane of the projection objective. This imaging property is compared with a target imaging property. Finally, the temperature of the immersion liquid is changed until the determined imaging property is as close as possible to the target imaging property.

Abstract: A method of optimizing an imaging performance of a projection exposure system is provided, wherein the projection exposure system comprises an illumination optical system for illuminating a patterning structure and a projection optical system for imaging a region of the illuminated patterning structure onto a corresponding field. The method comprises setting the field to a first exposure field, setting optical parameters of the projection exposure system to a first setting such that the imaging performance within the first exposure field is a first optimum performance, changing the field to a second exposure field, and changing the optical parameters to a second setting such that the imaging performance within the second exposure field is a second optimum performance.

Abstract: In order to optimize the image properties of several optical elements of which at least one is moved relative to at least one stationary optical element, the overall image defect resulting from the interaction of all optical elements is first of all measured. This is represented as a linear combination of the base functions of an orthogonal function set. The movable element is then moved to a new measurement position and the overall image defect is measured once again. After the linear combination representation of the new overall image defect, the image defects of the movable element and of the stationary element are calculated from the data thereby obtained. With only one movable optical element a target position in which the overall image defect is minimized can be directly calculated and adjusted there from. If several movable optical elements are available, methods are given for the efficient determination of the respective target position.

Abstract: In an immersion lithography apparatus or device manufacturing method, the position of focus of the projected image is changed during imaging to increase focus latitude. In an embodiment, the focus may be varied using the liquid supply system of the immersion lithographic apparatus.

Abstract: A method of adjusting a projection objective permits the projection objective to be adjusted between an immersion configuration and a dry configuration with few interventions in the system, and therefore to be used optionally as an immersion objective or as a dry objective. The projection objective has a multiplicity of optical elements which are arranged along an optical axis of the projection objective, the optical elements comprising a first group of optical elements following the object plane and a last optical element following the first group, arranged next to the image plane and defining an exit surface of the projection objective which is arranged at a working distance from the image plane. The last optical element is substantially without refracting power and has no curvature or only slight curvature.

Abstract: In a method for determining wavefront aberrations for the characterization of imaging characteristics in an optical imaging system, the measurement results from two different measurement methods, which are carried out at successive times, are combined. In this case, at least some of the aberration parameters which are determined in the previous first measurement method are used as a given precondition for determining aberration parameters with the aid of the second measurement method, and are assessed accordingly. This results in a hybrid method, in which the strength of at least two measurement methods are used in a combined form, and specific weaknesses of any one method can be avoided.

Abstract: In order to optimize the image properties of several optical elements of which at least one is moved relative to at least one stationary optical element, the overall image defect resulting from the interaction of all optical elements is first of all measured. This is represented as a linear combination of the base functions of an orthogonal function set. The movable element is then moved to a new measurement position and the overall image defect is measured once again. After the linear combination representation of the new overall image defect, the image defects of the movable element and of the stationary element are calculated from the data thereby obtained. With only one movable optical element a target position in which the overall image defect is minimized can be directly calculated and adjusted there from. If several movable optical elements are available, methods are given for the efficient determination of the respective target position.