By Nadir Jeevanjee

The moment variation of this hugely praised textbook presents an creation to tensors, staff concept, and their functions in classical and quantum physics. either intuitive and rigorous, it goals to demystify tensors by means of giving the marginally extra summary yet conceptually a lot clearer definition present in the maths literature, after which connects this formula to the part formalism of physics calculations. New pedagogical good points, reminiscent of new illustrations, tables, and boxed sections, in addition to extra “invitation” sections that offer available introductions to new fabric, provide elevated visible engagement, readability, and motivation for students.

Part I starts off with linear algebraic foundations, follows with the fashionable component-free definition of tensors, and concludes with functions to physics by using tensor items. half II introduces crew thought, together with summary teams and Lie teams and their linked Lie algebras, then intertwines this fabric with that of half I by way of introducing illustration thought. Examples and workouts are supplied in every one bankruptcy for reliable perform in making use of the offered fabric and techniques.

Prerequisites for this article comprise the normal lower-division arithmetic and physics classes, notwithstanding huge references are supplied for the prompted scholar who has no longer but had those. complex undergraduate and starting graduate scholars in physics and utilized arithmetic will locate this textbook to be a transparent, concise, and interesting creation to tensors and groups.

Reviews of the 1st Edition

“[P]hysicist Nadir Jeevanjee has produced a masterly booklet that might aid different physicists comprehend these topics [tensors and teams] as mathematicians comprehend them… From the 1st pages, Jeevanjee exhibits extraordinary ability find clean, compelling phrases to convey ahead the perception that animates the fashionable mathematical view…[W]ith compelling strength and readability, he offers many conscientiously worked-out examples and well-chosen particular difficulties… Jeevanjee’s transparent and forceful writing offers wide-spread circumstances with a freshness that would attract and reassure even a frightened pupil. [This] is a masterpiece of exposition and clarification that may win credits for even a professional author.”

—Physics Today

"Jeevanjee’s [text]is a necessary piece of labor on numerous counts, together with its exhibit pedagogical provider rendered to fledgling physicists and the truth that it does certainly provide natural mathematicians how to come to phrases with what physicists are announcing with an identical phrases we use, yet with an ostensibly diverse which means. The booklet is really easy to learn, very ordinary, choked with examples...and routines, and may do the activity the writer wishes it to do with style.”

—MAA Reviews

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Extra info for An Introduction to Tensors and Group Theory for Physicists

Example text

Vjv/ for the length (or norm) of v is sometimes used. ). Our reason for separating condition 4 from the rest of the definition will become clear when we consider the examples. One very important use of non-degenerate Hermitian forms is to define preferred sets of bases known as orthornormal bases. ei jej / D ˙ıij and are extremely useful for computation, and ubiquitous in physics for that reason. If . ei jej / D ıij and may be constructed out of arbitrary bases by the Gram–Schmidt process. If .

Feel free to introduce a basis to assist you in the proof. 9. v/ D 0 H) v D 0. Show that this is equivalent to T being one-to-one, which by the previous exercise is equivalent to T being one-to-one and onto, which is then equivalent to T being invertible. An important point to keep in mind is that a linear operator is not the same thing as a matrix; just as with vectors, the identification can only be made once a basis is chosen. For operators on finite-dimensional spaces this is done as follows: choose a basis B D fei gi D1:::n .

The converse to this is also true, and this is where the 19 See Rudin [16], for instance, for this and for proofs of all the claims made in this example. 39) nD 1 converges, yielding a square-integrable function g. 38). Now we know how to think about infinite-dimensional Hilbert spaces and their bases: a basis for a Hilbert space is an infinite set whose infinite linear combinations, together with some suitable convergence condition, form the entire vector space. 17. 36) of a Hilbert space basis is equivalent to our original definition of an (orthonormal) basis for a finite-dimensional inner product space V .

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