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Corrections to revised Second Edition (May 2014) of Student Friendly Quantum Field Theory
Note: 1st edition and 2nd edition (original) users also need to check this 2nd edition revision corrections page for additional corrections.
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Sorted by Page Number: This Page |
Sorted by Date Posted: Click Here |
Significant Corrections (may impact learning process)
Pg |
Chap |
Date Posted |
Significant Correction |
Reported by (blank = the author) |
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Nov 25, 2014 |
Solutions to Problems booklet now available. See problem solutions booklet . |
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22 |
2 |
June 16, 2015 |
Paragraph right before Sect 2.5.1. Replace entire paragraph/sentence with Note that, due to subtleties in the theory, non-relativistic chart relationships are most easily, and best considered at this point, expressed in Cartesian coordinates, where xi → Xi and pi = pi. |
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23 |
2 |
June 12, 2015 |
Box 2-2. My purpose in this box was to give a derivation of (B2-2.3) that was much simpler than that in other books. There are some subtleties involved, but it is best not to worry about them until after you have mastered QFT. If at that time, you feel up to it, check out Box2_2_comments |
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25-26 |
2 |
June 12, 2015 |
Line above (2-28) delete the minus sign after the equal sign. In (2-29), delete the minus sign before “i”. |
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30 |
2 |
June 16, 2015 |
(2-42) and (2-43): On RHS, insert (Cartesian system, where p j = pj = 3-momentum) (Correction posted on June 12, 2015 for these equations has been removed and replaced with this one.) |
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34 |
2 |
July 16, 2014 |
First line after (2-55). After “13.)”, insert Note from (2-55) that p^0 = gamma mc = E/c, where E is relativistic energy, and p^i = relativistic 3-momentum. |
Jimmy Snyder |
40 |
3 |
June 12, 2015 |
Eq (3-3). The subscript “i” on pi should be a superscript. |
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42 |
3 |
June 11, 2015 |
Eq (3-5). The subscript “i” on each pi should be a superscript. |
Doug McKenzie |
49-50 |
3 |
June 23, 2014 |
2nd line of text below (3.34), “(… Hermitian)”, should be (… Hermitian conjugate) . Same thing on pg. 50, just above (3-36). |
Jimmy Snyder |
53 |
3 |
Apr 23, 2015 |
There are some subtleties associated with (3-47) that merit more explanation in an Appendix. See Eq (3-47) subtleties, which includes the new Appendix E plus an elaboration. |
Michael Heiss |
68 |
3 |
Apr 23, 2015 |
Top line: “Appendix B” should be Appendix C |
John Davidson |
68 |
3 |
July 16, 2014 |
Sect 3.11.4, 3rd paragraph, next to last line: before “eigenstates”, insert linearly independent |
Jimmy Snyder |
79 |
3 |
July 16, 2014 |
(3-148), 4th (last) arrow, LHS: “x” should be x’ . Two places. |
Jimmy Snyder |
82 |
3 |
Jan 17, 2015 |
Prob 3, 1st line: Replace “(3-27)” with (3-25) -- |
Michael Heiss |
82 |
3 |
July 8, 2014 |
Prob. 3. Change “of negative unity” to is negative . One would have to assume a magnitude of unity, which would make sense if the value were positive. |
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90 |
4 |
Aug 27, 2014 |
Eq (4-27) was not explained clearly. On the RHS the integral is zero for p not = zero, but is V for p = 0. The spinor inner product in front of the integral is zero for p = 0. So, in any case, (4-27) is zero. |
Andrew Solomon |
118 |
4 |
June 12, 2014 |
Step 2 and Step 3 near top of page: “commutators” should be anti-commutators |
Sukruti Bansal |
121 |
4 |
July 16, 2014 |
(4-146), second line: insert a minus sign after the 2nd and 3rd equal signs. |
Holger Teutsch |
132 |
4 |
Aug 21, 2014 |
Prob. 14. Dr(p) should have a dagger on it. Also, just after that, insert in (4-29) |
Jimmy Snyder |
146 |
5 |
June 11, 2015 |
Eqs (5-45) and (5-46). The subscript “i” on each pi should be a superscript. |
Doug McKenzie |
147 |
5 |
Apr 21, 2015 |
In (5-50), the RHS should be summed over r, as it is done (correctly) in Wholeness Chart 5-4, pg. 156. |
Ben Balmforth |
180 |
6 |
Sept 15, 2014 |
Prob. 13. Delete part ii). Upon further reflection, I believe the logic there is flawed. Part i) suffices to make the point. |
Holger Teutsch |
211 to 212 |
7 |
Apr 21, 2015 |
It may be cumbersome keeping track of terms between (7-110) and (7-111). See From (7-110) to (7-111), which should help shortcut the tedium in doing so. |
Kurt Huddleston |
213c |
7 |
Sept 18, 2014 |
Prob. 11: At the end, before the period insert , if that commutator equals a constant |
Holger Teutsch |
233 |
8 |
Sept 18, 2014 |
In (8-85) delete the underbracket at the end under the polarization vectors. Replace the paragraph following that thru (8-86) with pg 233 revision . |
Holger Teutsch |
373 |
14 |
June 26, 2015 |
Prob. 3. Subscript C1 should be C2.. |
Jimmy Snyder |
288 |
11 |
June 19, 2014 |
Paragraph including (11-8) and (11-9): delete this paragraph and the associated margin note. The sign on E^2 in (11-8) is wrong and thus (11-8) does not equal the negative of energy density. This paragraph was as aside (not part of the theory development) and was intended to be a simple and intuitive insight into the LHS of (11-8). Unfortunately, the issue is neither simple nor intuitive, but delving into it in proper depth would take us off on a tangent away from the focus of the chapter. |
Bill Foster |
297 |
11 |
Sept 22, 2014 |
Above (11-40), add a footnote: The term “gauge covariant derivative” is different from, and should not be confused with, the “covariant derivative” of general relativity (and more generally, tensor analysis). It is unfortunate that similar nomenclature is used for the two cases. In the QFT we are studying, spacetime is flat (Minkowski space) and we use a Lorentz metric, so the covariant derivative of GR has Christoffel symbol of zero. This is made more confusing by the common dropping of the word “gauge” in QFT when referring to the gauge covariant derivative. You often have to glean the meaning from context. |
Thomas Fowler |
301 |
11 |
Aug 15, 2014 |
Prob. 9. To make things a little easier to understand: In 2nd line insert fermion before “field”. At end of last line, insert “Note that .” |
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329 |
13 |
Sept 16, 2014 |
(13-36). Exponent on e0 should be 4 not 2. Before that factor, insert a minus sign. |
Holger Teutsch |
393 |
15 |
Sept 22, 2014 |
(15-107). The fermion propagators need to be sandwiched between the vertex gamma matrices and the k in the denominator needs to have a slash through it. See (15-107) top row rev |
Holger Teutsch |
431a |
16 |
Sept 9, 2014 |
Last line: Change “and (16-17)” to (16-17), and (16-28) -- |
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431b |
16 |
Sept 9, 2014 |
End of 1st paragraph: After the equal sign, insert “g2” |
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421-423 |
16 |
Oct 31, 2014 |
Sect 16.4.6, Step #2 was not very clear. The revision, Sect 16.4.6 revision, should be considerably easier to understand. Note that Prob. 9 in this chapter is now deleted, as it related to material in Sect. 16.4.6 that was removed in this revision. |
Holger Teutsch |
431b |
16 |
Sept 22, 2014 |
Prob. 2 can be expressed more clearly with the following changes. 4th line: change “=” to goes to . Same line: after “interactions” insert , since there is no gμν in the scalar propagator . |
Holger Teutsch |
485 |
17 |
Oct 3, 2014 |
Prob. 3: The hint actually makes it more difficult. Do not express momentum as shown. Replace the hint with: “Use , a similar relation for particle #2, and the 3-momentum balance equation [where total 3-momentum is zero in the COM] to find . Divide this by the energy balance equation. Then add and subtract the energy balance equation from your result. “ |
Holger Teutsch |
491-509 |
18 |
July 21, 2014 |
Chap. 18 has some spots that needed more extensive explanations, and in one section, had a missing constant through several equations. The revised pages can be found at Chap 18 revised pgs. Red font indicates changed material. Note that the former appendix added little and has been replaced with a new appendix, which compares and contrasts the NRQM background for the path integral approach as handled by different texts. |
Luc Longtin helped in innumerable ways on this. Holger Teutsch and Christian Maennel also contributed |
503-504 |
18 |
June 12, 2014 |
An alternative derivation of the result in Sect. 18.9.2 may be easier to follow for some. See Alternative derivation for Sect. 18.9.2 |
Luc Longtin |
504-505 |
18 |
June 12, 2014 |
Line above (18-57), after comma at end of line, insert, where N = n + 1 = number of functions f_greek index , |
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505 |
18 |
June 12, 2014 |
(18-59): On RHS, delete factor of sq root (2 pi hbar). Delete middle expression completely. (18-60): Delete same factor in denominator. |
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506 |
18 |
July 18, 2014 |
Wholeness Chart 18-4, 1st column, 3rd row: Delete “(functionals)” |
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Minor Corrections (should not impact learning process)
Pg |
Chap |
Date Posted |
Minor Correction |
Reported by |
6 |
1 |
June 23, 2014 |
6th line: change “can not” to cannot |
Jimmy Snyder |
15 |
2 |
June 23, 2014 |
3rd line: change “M^0” to (MeV)^0, i.e., M=0 |
Jimmy Snyder |
22 |
2 |
June 23, 2014 |
Box 2-1, next to last paragraph, 2nd line: delete extra space and period before closing parenthesis. |
Jimmy Snyder |
23 |
2 |
June 23, 2014 |
3rd line of item 6 at the top of the page. "Box" should be Box 2.2 . |
Jimmy Snyder |
26 |
2 |
June 23, 2014 |
eqn (2.29), the S after the last equal sign is separated from the open bracket. |
Jimmy Snyder |
26 |
2 |
June 23, 2014 |
eqn (2.31) the size of the brackets is asymmetric. |
Jimmy Snyder |
26-28 |
2 |
June 23, 2014 |
eq (2-34): the superscript S is the wrong typeface, 2 places; eqn (2.37): ditto, 4 places; also in other places |
Jimmy Snyder |
27 |
2 |
June 23, 2014 |
Box 2.3, 3rd paragraph. Inspection is sufficient to reach these conclusions if H is hermitian, which it is. |
Jimmy Snyder |
27 |
2 |
June 23, 2014 |
Box 2.3, 4th line from the bottom. change "eigenstate state" to eigenstate |
Jimmy Snyder |
28 |
2 |
Sept 17, 2014 |
Wholeness Chart 2-4. Top RH box. All quantities between the bra and ket should be inside parentheses. |
Jimmy Snyder |
32 |
2 |
June 23, 2014 |
2nd line: “Preface” should not be capitalized |
Jimmy Snyder |
32 |
2 |
June 23, 2014 |
above (2.45), there should be a space between “See” and “Sect” and a period after “Sect” |
Jimmy Snyder |
32 |
2 |
July 16, 2014 |
The double bracket on the RHS of (2-47) should be a single bracket. |
Jimmy Snyder |
36 |
2 |
June 23, 2014 |
Prob. 4: First sentence at end, delete one period. Part c), remove period after first alpha subscript. |
Jimmy Snyder |
36 |
2 |
June 12, 2014 |
Prob. 4, 1st line: superscript “alpha beta” on “g” should be smaller font size. |
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43 |
3 |
June 23, 2014 |
2nd line below (3.9), the dagger is placed too far to the upper right of B_n. |
Jimmy Snyder |
44 |
3 |
June 23, 2014 |
Below (3.13) and also text below (3.15)(44), the dagger on B is misplaced. Three instances. |
Jimmy Snyder |
46 |
3 |
July 16, 2014 |
3rd line after (3-24): subscript “ k’ “ should have prime not apostrophe. |
Andrew Solomon |
53-54 |
3 |
Aug 20, 2014 |
Eqs (3-51), (3-52), (3-53) the omegas in the exponents should all be omega_k. |
Jimmy Snyder |
57 |
3 |
July 9, 2014 |
Above (3-65), after “examples,”, insert where k not equal k’, |
Jimmy Snyder |
57 |
3 |
July 9, 2014 |
Paragraph above Sect. 3.5 headin, 1st line, “of LHS” should be “of the LHS”. |
Jimmy Snyder |
58 |
3 |
July 9, 2014 |
In eqn (3-72), the underbracket is redundant given the text that follows it. |
Jimmy Snyder |
61 |
3 |
July 9, 2014 |
In the 2nd line on the page, there is an extra period after i.e., |
Jimmy Snyder |
61 |
3 |
July 9, 2014 |
Sect. 3.6.6, last paragraph, next to last line: “of this book”. should say of this book's publication |
Jimmy Snyder |
61 |
3 |
July 9, 2014 |
The title of section 3.7.1 should have a comma between “Currents” and “Operators”. |
Jimmy Snyder |
64 |
3 |
July 16, 2014 |
Sect. 3.8.3, 2nd line: delete extra space before “and” |
|
65 |
3 |
July 16, 2014 |
Chart 3-1; Fermions column, 3rd box under heading: delete “the”. |
Jimmy Snyder |
67 |
3 |
July 16, 2014 |
5th line below (3-112). Change“(not eigen)” to (not necessarily eigen) |
Jimmy Snyder |
69 |
3 |
July 16, 2014 |
Wholeness Chart 3-3, 3rd row under headings: Before “frequency” insert angular . |
Jimmy Snyder |
71 |
3 |
Apr 23, 2015 |
Second line; should be "(interaction).” rather than “(interaction.)” |
John Davidson |
74 |
3 |
July 16, 2014 |
Next to last line on pg. The subscript 0 on k should be smaller font. |
Jimmy Snyder |
75 |
3 |
July 16, 2014 |
In the text below (3-136), Insert a space between “see” and “(3-2)”. |
Jimmy Snyder |
75 |
3 |
July 16, 2014 |
paragraph to the right of Figure 3-5, 2nd line of text. Change “still c.c.w.” to still counter clock-wise [ccw], as in Fig. 3-4 |
Jimmy Snyder |
79 |
3 |
July 16, 2014 |
From (3-149) to (3-152) three different forms are used to symbolize the differential element in 3D position space, dx, d3x, and d3x. These should all be the same for consistency. Take your pick. |
Jimmy Snyder |
82 |
3 |
June 23, 2014 |
Prob. 2: the dagger on B is misplaced; Prob. 3: dagger on B_k is misplaced |
Jimmy Snyder |
82 |
3 |
Aug 21, 2014 |
Prob. 12, 5th line: after “different from” insert (orthogonal to) |
Jimmy Snyder |
92 |
4 |
Apr 23, 2015 |
Eq (4-36) under bracket: “(p)” should be just after "u_r-dagger” not after gamma^0. |
John Davidson |
94 |
4 |
Nov 3, 2014 |
Box 4-1: 4th and 5th eqs need to be aligned with others |
|
107 |
4 |
June 12, 2014 |
Box 4-3: Equation numbers need to be aligned. |
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115 |
4 |
Apr 23, 2015 |
Second line of section 4.9.2: move period in "… pseudo-vector).” inside parenthesis. |
John Davidson |
122 |
4 |
June 12, 2014 |
exponents should be larger font size. |
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127 |
4 |
June 12, 2014 |
Conclusion #2: Remove underlining on whole sentence. Leave underlining on “Conclusion #2” |
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133 |
4 |
Aug 21, 2014 |
Prob. 25. Change period at end to question mark. |
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143 |
5 |
Apr 23, 2015 |
3rd line below Fig. 5-2: In "del X A”, “X" needs to be reformatted. |
John Davidson |
148 |
5 |
June 12, 2014 |
(5-54) and (5-56): “a” and “b” should be larger font. |
|
149 |
5 |
Apr 23, 2015 |
4th side note: 1st “RQM” should be QFT |
John Davidson |
150 |
5 |
June 12, 2014 |
(5-68): k^2 in denominator should be larger font size. |
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151 |
5 |
Apr 23, 2015 |
Eq (5-69): ik_mu RHS has different font point sizes. |
John Davidson |
151 |
5 |
Apr 23, 2015 |
Ref to original papers by Gupta and Bleuler should be added: K. Bleuler, Eine neue Methode zur Behandlung der longitudinalen und skalaren Photonen, Helvetica Phys. Acta 23 (1950), 567586. S.N. Gupta, Theory of longitudinal photons in quantum electrodynamics, Proc. Phys. Soc. Sect.A. 63 (1950), 681691. |
John Davidson |
156 |
5 |
June 12, 2014 |
Wholeness Chart 5-4, 2nd row of cells from bottom: exponent “ikx” should be smaller font size. |
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179 |
6 |
Aug 27, 2014 |
Probs. 1, 2, 4, and 6: Font for primes should be changed so they look more like primes than superscript commas. |
Holger Teutsch |
180 |
6 |
Aug 27, 2014 |
Prob. 12, end of 3rd line: gamma^mu should be larger font. |
|
183 |
7 |
June 12, 2015 |
Sect. 7.1.1, second line: “Gaussian” should be “Heaviside-Lorentz”. |
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184 |
7 |
Apr 23, 2015 |
Eq (7-13): subscript “I” should be italic |
John Davidson |
185 |
7 |
Apr 23, 2015 |
Eq. (7-15): Last underbracket superscript “I” should be 1. |
John Davidson |
188 |
7 |
Sept 17, 2014 |
Wholeness Chart 7-1. RH column for SP, HP, and IP.. All quantities between the bra and ket should be inside parentheses. |
Jimmy Snyder |
192 |
7 |
Sept 17, 2014 |
(7-39). All quantities between the bra and ket should be inside parentheses. |
Jimmy Snyder |
211 |
7 |
Apr 21, 2015 |
In (7-110) first term in middle row, underbracket relation. The [A1d,C3c] should be [A1d,C3c]-/+, i.e., it should have minus/plus subscript as all other brackets in the equation do. |
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219 |
8 |
June 23, 2014 |
Box 8.1, last paragraph, 1st sentence: delete extra period |
Jimmy Snyder |
222 |
8 |
Apr 23, 2015 |
Eq (8-30), last row: under bracket should not include d^4k |
John Davidson |
233 |
8 |
July 2, 2014 |
(8-85) and (8-86): “delta^ (k k′)” should be delta^(4) (k k′) |
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233 |
8 |
Nov 3, 2014 |
6th line up from bottom: insert hyphen after “4”. |
|
235 |
8 |
Sept 18, 2014 |
(8-89) should have a minus sign for the RHS |
Holger Teutsch |
236 |
8 |
Oct 6, 2014 |
B. 4., end of 2nd line: Insert “r represents spin state for fermions and polarization state for photons, ( (4-93) and (4-94), pg. 111, may be of help below),” |
Thomas Fowler |
255 |
9 |
July 16, 2014 |
(9-3) 2nd line: parenthesis before N should be non italic. at end of last line: add )d4x1 d4x2 d4x3 |
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256 |
9 |
Apr 23, 2015 |
3rd line: the x_i should be a subscript to the (…) term rather than in-line with it. |
John Davidson |
265 |
9 |
Oct 28, 2014 |
Wholeness Chart 9-1: Top row, make arrow non italic. |
|
265 |
9 |
June 12, 2014 |
Prob. 1, at end: Change period to question mark. |
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274 |
10 |
June 19, 2015 |
In (10-8) and throughout this sections, change N to script N (representing number density per unit k. |
|
277 |
10 |
June 12, 2014 |
1st margin note: Delete space between “usual” and “type” |
|
285a |
10 |
Dec 24, 2014 |
eq (10-37): make “lim” symbol smaller font |
|
305 |
12 |
June 12, 2014 |
6th and 7th bullets: alpha and pi should be smaller size. |
|
305 |
12 |
June 12, 2014 |
Under (12-1): in ket, remove space after “f”. |
|
316 |
12 |
June 12, 2014 |
Paragraph above Fig. 12-4: “Figure” should be “Fig.” |
|
323 |
13 |
Apr 23, 2015 |
Eq (13-5): A(lambda, m) goes to - infinity rather than + infinity. |
John Davidson |
325 |
13 |
Apr 21, 2015 |
Gordon’s identity (13-18) should have a box around it, as it is important in a number of places in subsequent chapters. But, it is not worth trying to memorize it. |
|
343 |
14 |
Apr 23, 2015 |
line 2: change ”,to” to to, |
John Davidson |
350 |
14 |
June 12, 2014 |
Wholeness Chart 14-1: After heading “Short cut route”, “Sect. 0” should be Sect. 14.2.3 |
|
372 |
14 |
Sept 17, 2014 |
(14-99). The e’s inside the bra and ket should be primed. |
Holger Teutsch |
403 |
16 |
June 12, 2014 |
top line: lower case “phi” should be upper case “Phi”. 2 places. |
|
405 |
16 |
Oct 28, 2014 |
Fig. 16-1: Correct spacing on figure title. (Only occurred in May 2014 revision, not earlier versions.) |
|
419 |
16 |
June 12, 2014 |
(16-72) and (16-72): (2 pi)^3 in denominators should be larger font size. 3 places |
|
422 |
16 |
Oct 28, 2014 |
Eq (16-83): Delete one of the two periods at the end |
|
429 |
16 |
Apr 23, 2015 |
Last line of paragraph starting with “Rather…”, move period in ”.)” to outside of parenthesis. |
John Davidson |
431b |
16 |
Sept 9, 2014 |
3rd line: change “[1 1 0 0]” to -- [1 1 0 0]T -- |
|
485 |
17 |
Sept 9, 2014 |
Problem 1, 3rd line: After “Find” insert the --. |
|
485 |
17 |
Oct 3, 2014 |
Prob 3, 2nd line, 1st word: Delete “s” at end of “particles”. |
|
493 |
18 |
Apr 23, 2015 |
2nd line after eq (18-19), end of line: Period should be outside parenthesis. |
John Davidson |
504 |
18 |
June 12, 2014 |
(18-52): subscript “a” should be alpha . 2 places. Also “dx” too small, 3 places. |
|
504 |
18 |
Oct 28, 2014 |
Eq. (18-55): In the exponent, delete spaces on either side of “delta t” |
|
506 |
18 |
Oct 28, 2014 |
2nd line: delete “quantum field theory” |
|
506 |
18 |
July 18, 2014 |
Wholeness Chart 18-4, 1st column, 3rd row: change “Dynamic” to Dynamical . 2 places. |
|
506 |
18 |
July 18, 2014 |
Wholeness Chart 18-4, 1st row: change “phidot” to phi,_mu |
|
507 |
18 |
July 18, 2014 |
Wholeness Chart 18-4, 1st column, 3rd row: change “Dynamic” to Dynamical |
|
507 |
18 |
July 18, 2014 |
Wholeness Chart 18-4, 2nd part “Quantum Theories”, 3rd column, 4th row: change “phidot” to phi,_mu |
|
514 |
19 |
Oct 6, 2014 |
B. 4., end of 2nd line: Insert “r represents spin state for fermions and polarization state for photons, ( (4-93) and (4-94), pg. 111, may be of help below),” |
Thomas Fowler |
522 |
index |
Oct 6, 2014 |
After “Feynman rules, 224, 236, 513”, insert , 514 . |
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