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only be read by the receiver and no one else in the middle will be able to decode it Currently the pro les specify two possible mechanisms for implementing secure transport connections over a network: TLS (transport layer security 10) and ISCL (integrated secure communication layer V100) It endows DICOM with a limited set of features that are required for implementation 17413 Digital Signature Pro les Although the secure transport connection protects the data during transit, it does not provide any lifetime integrity checks for DICOM SOP (service-object pair) instances The digital signature pro les published in 2001 provide mechanisms for lifetime integrity checks using DS DS allow authentication of the identity entity that created, authorized, or modi ed a DICOM data set This authentication is in addition to any authentication done when exchanging messages over a secure transport connection.

5

The only trick to successfully complete this exercise is to remember that the top-left corner of an image is (0,0). This means that you must remember to subtract 1 from the width and height of the image to get the rightmost position and bottommost position of the image, respectively. Here s the code to draw the black border:

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Except for a few attributes, the pro les do not specify any particular data set to sign The creator of a DS should rst identify the DICOM data subset, then calculate its MAC and hash value, and last, sign the MAC into a DS As with any DS, the receiver can verify the integrity of this DICOM data subset by recalculating the MAC and comparing it with the one recorded in the DS Typically the creator of the DS would only include data elements that had been veri ed in the MAC calculation for the DS The image digital envelope described in Section 173 has a very large data set that includes the segmented image and relevant patient information in the DICOM header.

Note that both Eqs. (14.193) and (14.194) involve the maniupulation of wavefronts that derive from the rotation of the part and the rotation of the wavefront data matrices by 180 . This allows the separation of even and odd errors in the interferometer when we have access to the cat s eye con guration. Figure 14.56b shows the results of such calibration calculations as well as the individual and composite errors in the interferometer and test part. This method is usually employed when it is essential to achieve the very highest accuracies possible. The method is only effective when the is operated in a stable environment and the 0 and 180 test part con gurations of W1 and W2 match the pixel coordinates x0 ; y0 and x0 ; y0 of the detector matrix. This calibration procedure is conveniently carried out with PSIs that can easily manipulate and store wavefronts in memory. Errors incurred by improper alignment of the various surfaces have been examined by Truax (1988) and Elssner et al. (1989). Generally, lateral alignments are the most critical and need to be held to within one pixel or less. The special case of at surfaces can be calibrated by using three surfaces in different orientations. A similar approach has been applied to Fizeau reference calibration (Schulz and Schwider, 1976). The use of Zernike polynomials facilitates the calibration process for ats (Fritz, 1984).