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The Condition class wraps a lock. You can pass a Lock object to the Condition constructor; if not, it creates an RLock internally. A condition object has acquire() and release() methods, which wrap those of the underlying lock object. Condition objects have other methods: wait([timeout]), notify(), and notifyAll(). A thread should acquire the lock before calling these methods. A call to the wait([timeout]) method immediately releases the lock, blocks until notification is received (when another thread calls notify() or notifyAll()), acquires the lock again, and then returns. If you supply a value for timeout, the call will return after that many seconds have passed, whether or not it was notified or reacquired the lock. You call notify to wake up other threads that have called wait on the condition. If there are waiting threads, notify awakens at least one of them. (Currently, notify never awakens more than one, but this is not guaranteed for future versions.) notifyAll wakes up all the waiting threads.

2 Im(Y11)

+ p and what if Ew, = p Derive an unbiased estimator for the variance of the w, if Ew, = + p and if

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The imaging detectors, whether for point mapping, line scanning, or array detection, can be coupled with different types of spectrometers. Instrument types are classi ed by wavelength selection modality into imaging Fourier transform (FT) and tunable lter (TF) spectrometers, both of which are presented below, and dispersive spectrometers. FT imaging systems are classical laboratory instruments while TF spectrometers are compact and robust systems for chemical imaging. FT Spectrometers FT spectrometers (Figure 3) differ from scanning spectrometers by the fact that the recorded signal is an interferogram [14] (see 6.2). They can be coupled to a microscope or macrochamber with an FPA detector. FT chemical imaging systems (CISs) are available for Raman, NIR, and IR spectroscopy. However, they can only be considered as research instruments. For example, most IR imaging systems are FT spectrometers coupled to microscopes. This type of spectrometer allows the acquisition of spectra in re ection, attenuated total re ection (ATR), or transmission mode. TF Systems A TF is a device whose spectral transmission can be controlled by applying a voltage or acoustic signal. There are two main TF devices: acousto-optical TF (AOTF), based on diffraction, and liquid crystal TF (LCTF), based on birefringence. An AOTF is a transparent crystal in which an ultrasonic wave eld is created,

To write a multipart message, first call startmultipartbody(subtype [,boundary[,plist[,prefix]]]). The content-type header has main type multipart, subtype subtype, and any extra parameters you pass in plist. For each part of the message, call nextpart to get a MimeWriter for that part. After finishing each part of the message, call lastpart to finish the message off. The call to startmultipartbody also returns a filelike object; it can be used to store a message for non-MIME-capable software.

Summary

Public key cryptography is both slow and computationally taxing due to the long key lengths used by the RSA encryption scheme (typically 1024 bits in length). For this reason, most public key systems make use of what is known as a session key to encrypt or digitally sign messages. In the case of digitally signing a message, a one-time session key (usually 128 bits long) is used to sign the hash value attached to the message; then, the session key is encrypted by the sender s private key and included with the message as well. When the recipient receives the message, they use the sender s public key to decrypt the session key and then use the session key to decrypt the hash value. This method makes public key cryptography more efficient, as its takes much less time to encrypt or decrypt a session key than it would to perform the process on an entire e-mail message, attachments, and so forth. For the sake of clarity, use of session keys is assumed throughout this chapter when not explicitly mentioned.

P The maximum likelihood estimator (61, b2) of (PI,2 ) maximizes (6.63)while the corresponding maximum likelihood estimator 6 of a: is (6.62) with (&,&) substituted for

Low-luminance tritanopia is a phenomenon whereby observers with normal color vision become more and more tritanopic (yellow blue de cient) as luminance decreases since the luminance threshold for short-wavelengthsensitive cones is higher than that for the other two cone types. As can be seen in Equation 12.36, Ft is essentially 1.0 for all typical luminance levels. It approaches zero as the adapting luminance LA approaches zero, forcing the yellowness blueness response to decrease at low luminance levels. This factor is also of little importance in most practical situations, but necessary to model appearance over an extremely wide range of luminance levels. For most applications, it is better to avoid this situation by viewing samples at suf ciently high luminance levels. Given the yellowness blueness and redness greenness responses de ned above, an overall chromatic response M is calculated as their quadrature sum as shown in Equation 12.37. M = (M 2 + M 2 )1/2 YB RG (12.37)

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