By Harvey A. Ziessman MD, Janis P. O'Malley MD

ISBN-10: 0323029469

ISBN-13: 9780323029469

The third version of this profitable source maintains to provide a simple and reasonable option to grasp middle wisdom and evaluate very important evidence pertinent to the strong point. A concise, trouble-free format-with at-a-glance illustrations, containers, and tables-enables you to entry details speedy. Revised all through to mirror the very newest advances within the box, it makes a very good learn resource for certification and recertification evaluation in addition to scientific reference.Presents transparent descriptions of nuclear drugs rules and techniques.Emphasizes the center wisdom wanted for certification and perform in a transparent and succinct manner.Offers pattern protocols for every procedure.Provides a great source at a cheap price.Presents revised Nuclear Cardiology, Neurology, Endocrine procedure, and Genitourinary procedure chapters that replicate the swift enlargement of puppy imaging, together with an entire new bankruptcy on F-18 FDG puppy imaging.Features accelerated use of Pearls, Pitfalls, and regularly requested Questions for extra useful details.

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Additional info for Nuclear Medicine: The Requisites, Third Edition

Example text

In any setting where a quantitative measurement is required, such as determining the amount of radioactivity in a radiopharmaceutical to be given to the patient or in a blood sample used in calculating a physiologic parameter or performing quality control of nuclear instrumentation, estimates of statistical certainty are necessary. Radioactive decay follows Poisson statistics or the Poisson probability law. The Poisson probability density function is similar but not identical to the Gaussian or normal probability density function.

The Poisson probability density function is similar but not identical to the Gaussian or normal probability density function. Curves expressing the Poisson and Gaussian probability density functions are more closely matched as the number of observed events is increased and practically identical if the mean is greater than 20. For data obeying the Poisson probability distribution, the standard deviation (SD) is given by SD = r , where r is the true mean. Because the true mean is usually estimated from an average of a number of individual measurements, the estimated standard deviation is SD(est) = r (es).

28 NUCLEAR MEDICINE: THE REQUISITES resolution is also lost through difficulty in collimating high-energy photons. Characteristic Radiation and Auger Electrons When an orbital electron is removed from its shell, it leaves a vacancy that is rapidly filled by a free electron or an electron from a shell farther from the nucleus. In this process,the “cascading”electron gives up energy as it fills in the vacancy and becomes more tightly bound. Most often, the energy that is given up by the electron is emitted in the form of electromagnetic radiation.

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Nuclear Medicine: The Requisites, Third Edition by Harvey A. Ziessman MD, Janis P. O'Malley MD


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