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0n 1 0 1 0ff 0n 1 1 0 0ff 0n 0ff 0 1 1 0n How do you build a 2-input NOR Gate? L2: 6.111 Spring 2006 Introductory Digital Systems Laboratory 11 Theorems of Boolean Algebra (I) Theorems of Boolean Algebra (I) (cid:132) Elementary 1. X + 0 = X 2. X + 1 = 1 3. X + X = X 4. (X) = X 5. X + X = 1 (cid:132) Commutativity: 6....
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Z) = X • (Y + Z) (cid:132) Consensus: 12D. (X + Y) • (X + Z) = X + (Y • Z) 13. (X • Y) + (Y • Z) + (X • Z) = X • Y + X • Z 13D. (X + Y) • (Y + Z) • (X + Z) = (X + Y) • (X + Z) (cid:132) De Morgan's: 14. (X + Y + ...) = X • Y • ... 14D. (X • Y • ...) = X + Y + ... (cid:132) Generalized De Morgan's: 15. f(X1,X2,...,Xn,...
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A B Cin + A B Cin + A B Cin (cid:132) Product term (or minterm) (cid:134) ANDed product of literals – input combination for which output is true (cid:134) Each variable appears exactly once, in true or inverted form (but not both) L2: 6.111 Spring 2006 Introductory Digital Systems Laboratory 14 Simplify Boolean Expr...
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B, C) = Σm(1,3,5,6,7) = m1 + m3 + m5 + m6 + m7 F = canonical form ≠ minimal form A B C + A B C+ A B C + A B C + ABC F(A, B, C) = A B C + A B C + AB C + ABC + ABC = (A B + A B + AB + AB)C + ABC = ((A + A)(B + B))C + ABC = C + ABC = ABC + C = AB + C (cid:132) Sum term (or maxterm) - ORed sum of literals – input combin...
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maxterm shorthand replace minterm indices with the indices not already used E.g., F(A,B,C) = Σm(3,4,5,6,7) = ΠM(0,1,2) 2. Maxterm to Minterm conversion: rewrite maxterm shorthand using minterm shorthand replace maxterm indices with the indices not already used E.g., F(A,B,C) = ΠM(0,1,2) = Σm(3,4,5,6,7) 3. Minterm expan...
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A has a different value in the two rows – A is eliminated L2: 6.111 Spring 2006 Introductory Digital Systems Laboratory 18 Boolean Cubes Boolean Cubes (cid:132) Just another way to represent truth table (cid:132) Visual technique for identifying when the uniting theorem can be applied (cid:132) n input variables = n-...
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A The on-set is completely covered by the combination (OR) of the subcubes of lower dimensionality - note that “111” is covered three times L2: 6.111 Spring 2006 Introductory Digital Systems Laboratory 20 Higher Dimension Cubes Higher Dimension Cubes 011 111 010 B C 110 001 101 000 A 100 F(A,B,C) = Σm(4,5,6,7) on-set...
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, 11, 10 (only a single bit changes in code for adjacent map cells) 2-variable K-map 0 1 0 1 2 3 B A 0 1 AB A C 00 01 11 10 3-variable K-map 0 1 0 1 6 7 4 5 2 3 B AB CD 00 01 11 10 C A 00 01 11 10 0 1 3 2 4 5 7 6 B 12 13 8 9 15 11 14 10 D 4-variable K-map L2: 6....
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1 1 0 0 1 1 B F(A,B,C,D) = Σm(0,2,3,5,6,7,8,10,11,14,15) F = C + A B D + B D Find the smallest number of the largest possible subcubes that cover the ON-set 0011 0010 C 0001 0000 D A B 0111 1010 0110 0101 0100 1000 1011 1111 1110 K-map Corner Adjacency Illustrated in the 4-Cube 1001 1101 1100...
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B L2: 6.111 Spring 2006 Introductory Digital Systems Laboratory 25 Hazards Hazards AB C 00 01 11 10 0 1 0 0 0 1 1 1 1 0 F A C B Implemented with MSI gates: '00 '00 '00 1 '00 F 2 Static hazards: Consider this function: F = A * C + B * C A C B A = B = 1 C 1 2 F Gate delay Glitch L2: 6.111 Spring 2006 Introductory Digit...
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2.3.2 Swollen (coil) polymers in good solvents Most of the terms in the trial free energy of Eq. (2.49) have definite sign. The exception is the term proportional to N 2(a/R)3 which has opposing contributions from the repulsive 1/2). The sign of this term and attractive parts of the potential, and is proportional to (χ ...
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ization group theory is to estimate the exact value of ν = 0.591 . . . , remarkably close to the Flory approximation of 3/5. While not directly relevant to real polymers, it is possible to inquire about the exponent ν for self-avoding walks in d-spatial dimensions– e.g., for polymers confined to a d = 2 dimensional surf...
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− 2χ 1 − 2 ρ + ρ2 6 + higher order terms. (2.54) The optimal density for T < θ is obtained by minimizing the above free energy, leading to 1 N d ln Z dρ − = 1 2 − (cid:18) χ + (cid:19) ρ 3 + , · · · ρ = 3 χ (cid:18) + , · · · (cid:19) 1 2 − 42 (2.55) i.e. a density that vanishes linearly on approaching the θ-temperatu...
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can be visualized as the collection of all maximally compact configurations. In a lattice version, these are self-avoiding walks that visit all sites, leaving no empty ones, and are referred to as Hamiltonian walks. The number of Hamiltonian walks also grows exponentially with the number of steps as g′N , but is much sm...
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αic = NBh V 2 abic ≡ Nσ2 , (2.60) h , where noting that NB = (z have folded the proportionality constant into the definitions of ε0 and σ2. − 44 For large N, the probability distribution for the energy will take the Gaussian form p(E) = 1 √2πNσ2 exp (E Nε0)2 − 2Nσ2 . (cid:21) − (cid:20) (2.61) Since the total number of...
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− Ec (cid:18) Nε0 Ec − Nσ2 = kB (cid:19) √2 ln g′ σ ⇒ kBTC = σ √2 ln g′ . (2.64) There are presumably a few low energy states with energy close to Ec, and the system freezes into one of these for T Tc. (cid:12) (cid:12) (cid:12) (cid:12) ≤ 45 2.3.5 Designed REM for protein folding It is tempting to equate the freezing...
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Nε0)2/(2Nσ2) En . (2.65) As depicted in the figure, the above result equates the slope of the tangent line from the point at En computed in two different ways. To justify the above result, note that in the canonical ensemble, the probability of finding the system in the native state is pn = e−βEn Z(β) , with Z(β) = e−βEn ...
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Noise in Cascaded Amplifiers F1,G1 F2,G2 1 2 ≡ 3 1 F1+2,G 1+2 3 F ∆+ 2 1 NS 1 1 NS 3 3 where S 3 = S G G 121 N 2 = kT G F 1 o 1 ⎛ ⎜ Recall ⎜ ⎝ F 1 = N 3 = G kT 2 G F + 1 1 o ( FG 22 ⎞ ⎟ ⎟ ⎠ NS 1 1 NS 2 2 ) o 1 kT − amplified from “2” excess from “2” ∴ NS 3 3 = S G G 1 ...
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… cascade noise formula A B vs. B A The better choice is not obvious. F1,2 also depends on interstage impedance mismatches and gain of the first amplifier, not just on F1 L2 Noise in superheterodyne receivers 0 f fo Gc,Fc S1,N1 S2,N2 × 0 fi.f. f L.O. “lower (rf) sideband” Gi.f.,Fi.f. ∆ “i.f.”...
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amp. 2 −≅ ( 3 ~ 8 − 9 ) dB L4 Basic receiver types-Amplification 1) Simple detector B f ( )2 h(t) vo(t) 2) RF Amplifier 3) Superheterodyne OR OR × N1 1) 2) 3) 4) Basic receiver types-Combinors vo(t) Total power radiometer vo(t) Dicke radiometer × vo(t) Multiplication (correlation) receiver ...
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) The scattering matrix S is defined only when the n-port is imbedded in a network 2) The phases of a i and bi can be defined as some linear combinations of those for voltage and current .g.e a i V = + 2Y o = ( V + ) I Z o , Z 8 o b i = ( V − ) I Z o Z 8 o P1 Gain definition for N-port networks “Trans...
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= k(T1 +T2) ∗ t a =•⇒ bba ∗ t 00 ⎡ ⎢ 00 ⎢ ⎢ ⎣ α βαα α ⎤ ⎥ ⎥ ⎥ ⎦ ∗ t b b =• ∗ ( aS t ) ( aS • ) • = ∗ t ∗ t Sa aS Therefore ∗ t ISS == 001 ⎤ ⎡ ⎥ ⎢ 010 ⎥ ⎢ 100 ⎥ ⎢ ⎦ ⎣ ; if the combiner is lossless P4 Example of constrained N-port networks ; if the container is lossless Therefore ∗ t I...
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atisfied simultaneously for this system Ideal matched 2-input-port combiners are impossible P5 Another N-port network example Can we match all 3 ports simultaneously? 1 2 3 (Note: S is defined only when imbedded in network) For 3 matched ports: S = 0 ⎡ ⎢ α ⎢ β ⎢ ⎣ βα 0 ⎤ ⎥ γ ⎥ 0 ⎥ ⎦ γ Does ∗ t ...
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matched 3 4 We can show ∆φ for 1 3 versus 1 4 paths is unique using losslessness, reciprocity, and symmetry P8 signal + S(t ) + (cid:65) (t) V = local oscillator Th - Mixer vTh - + vo(t) Rs i(t) RL i o = V Th ( R R + S L ) >> i(t) i diode: sin +ω o vt s sin ω s t i ≅ v 2 d for )t(v ...
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(Note: 4 v ⇒ d . f.f 2 i , can be in i.f. passband) Normally: a 4-port model suffices to find F,T " , : " T R SSB signal image 1 2 4 3 output internal noise R2 Mixer Noise Figure Using 4-port Model T R = T SSB = T)1F( − o = T o ( t L rc − )1 signal for single sideband (SSB) operation image ...
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2 signal S 43 2 S 41 image Both ports 1 and 2 are signal, so S 4 = kT o ( 2 + S S 41 2 ) ( S1 − 42 output 1 2 4 3 internal noise )2 44 It follows that T DSB = T 3 S 43 2 [ S 2 41 + S 2 42 ] Often suggested: SSBF ≅ F2 DSB R4 Double-sideband Receiver Therefore T SSB = T 2 S...
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6.825 Techniques in Artificial Intelligence Resolution Theorem Proving: Propositional Logic • Propositional resolution • Propositional theorem proving • Unification Lecture 7 • 1 Today we’re going to talk about resolution, which is a proof strategy. First, we’ll look at it in the propositional case, then in the...
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that that one rule is all you need to prove things. At least, to prove that a set of sentences is not satisfiable. So, let's see how this is going to work. There's a proof strategy called Resolution Refutation, with three steps. And it goes like this. 4 Propositional Resolution • Resolution rule: α v β β v γ ¬...
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right? If you assert that the negation of the thing that you're interested in is true, and then you prove for a while and you manage to prove false, then you've succeeded in a proof by contradiction of the thing that you were trying to prove in the first place. So you run the resolution rule until you derive false o...
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So let's just do a proof. Let's say I'm given “P or Q”, “P implies R” and “Q implies R”. I would like to conclude R from these three axioms. I'll use the word "axiom" just to mean things that are given to me right at the moment. 9 Propositional Resolution Example Step Formula Derivation 1 P v Q Given Prove R 1 ...
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. We'd like to prove that R follows from these things. But what we're going to do instead is say not R, and now we're trying to prove false. And if we manage to prove false, then we will have a proof that R is entailed by the assumptions. 13 Propositional Resolution Example Prove R 1 P v Q 2 R P → Q 3 R →...
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16 Propositional Resolution Example Prove R 1 P v Q 2 R P → Q 3 R → Step Formula Derivation 1 2 3 4 5 6 7 P v Q P v R Q v R R ¬ ¬ ¬ Q v R P ¬ Q ¬ Given Given Given Negated conclusion 1,2 2,4 3,4 Similarly, we can take lines 3 and 4, resolve away R, and get “not Q”. Lecture 7 • 17 17 Proposit...
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desired contradiction. 19 Propositional Resolution Example Step Formula Derivation Prove R 1 P v Q 2 R P → Q 3 R → false v R R v false ¬ false v false 1 2 3 4 5 6 7 8 9 P v Q P v R Q v R R ¬ ¬ ¬ Q v R P ¬ Q ¬ R • Given Given Given Negated conclusion 1,2 2,4 3,4 5,7 4,8 Lecture 7 • 20 Ho...
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Lecture 7 • 22 22 The Power of False Step Formula Derivation Prove Z P1 P 2 ¬ It does, and it’s easy to prove using resolution refutation. Lecture 7 • 23 23 The Power of False Prove Z P1 P 2 ¬ Step Formula Derivation 1 2 3 P ¬ ¬ P Z Given Given Negated conclusion We start by writing down the ass...
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are very brittle. Lecture 7 • 27 So, we see, again, that any conclusion follows from a contradiction. This is the property that can make logical systems quite brittle; they’re not robust in the face of noise. We’ll address this problem when we move to probabilistic inference. 27 Example Problem Convert to CNF ...
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R ¬ R) Æ ( ¬ P v R) Lecture 7 • 30 The second turns into (“P or R” and “not P or R”). We probably should have simplified it into “False or R” at the second step, which reduces just to R. But we’ll leave it as is, for now. 30 Example Problem Convert to CNF Prove R 1 2 3 (P (P → → Q) → Q P) → R (...
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Q P) → R (R 3 → S) (S → ¬ → Q) 1 2 3 4 5 6 7 P v Q P v R ¬ R v S R v P v R Q ¬ S v Q ¬ R ¬ ¬ Neg Lecture 7 • 32 Now we can almost start the proof. We copy each of the clauses over here, and we add the negation of the query. Please stop and do this proof yourself before going on. 32 Resolut...
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a shorter clause. And the shorter a clause is, the closer it is to false. 35 Proof Strategies • Unit preference: prefer a resolution step involving an unit clause (clause with one literal). • Produces a shorter clause – which is good since we are trying to produce a zero-length clause, that is, a contradiction....
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to move to the first-order case. And there's going to be a resolution rule in the first-order case, and it's essentially the same inference rule, but the trick is what to do with the variables. And what to do with the variables is pretty hard and pretty complicated. We’ll spend the rest of this lecture understandin...
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) Q(A) Syllogism: All men are mortal Socrates is a man Socrates is mortal uppercase letters: constants lowercase letters: variables x. ¬ ∀ P(x) v Q(x) P(A) Q(A) Equivalent by definition of implication P(A) v Q(A) ¬ Substitute A for x, still true P(A) Q(A) then Propositional resolution Lectur...
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y. We can think about different ways that we can substitute terms into this expression, right? Those are called substitution instances of that expression. 45 Substitutions P(x, F(y), B) : an atomic sentence Substitution instances Substitution {v1 /t1,…, vn /tn} Comment Lecture 7 • 46 A substitution is a set ...
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phabetic variant To get P(G(z), F(A), B), we substitute the term G(z) in for x and the constant A for y. Lecture 7 • 49 49 Substitutions P(x, F(y), B) : an atomic sentence Substitution instances P(z, F(w), B) Substitution {v1 /t1,…, vn /tn} {x/z, y/w} P(x, F(A), B) {y/A} P(G(z), F(A), B) {x/G(z), y/A} Co...
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B) : an atomic sentence Substitution instances P(z, F(w), B) Substitution {v1 /t1,…, vn /tn} {x/z, y/w} P(x, F(A), B) {y/A} P(G(z), F(A), B) {x/G(z), y/A} Comment Alphabetic variant P(C, F(A), B) {x/C, y/A} Ground instance Applying a substitution: subst({A/y},P(x, F(y), B)) = P(x, F(A), B) P(x, F(y), B) {A...
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ifiers s ω1 s ω2 s So, let’s look at some unifiers of the expressions x and y. Since x and y are both variables, there are lots of things you can do to make them match. Lecture 7 • 55 55 Unification • Expressions ω1 and ω2 are unifiable iff there exists a substitution s such that ω1 s = ω2 s • Let ω1 = x and ω...
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= ω2 s • Let ω1 = x and ω2 = y, the following are unifiers s {y/x} {x/y} ω1 s ω2 s x y x y {x/F(F(A)), y/F(F(A))} F(F(A)) F(F(A)) {x/A, y/A} A A Or, you could substitute some constant, like A, in for both x and y. Lecture 7 • 59 59 Most General Unifier Lecture 7 • 59 Of the unifiers we considered on the pre...
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such that ω1 s = (ω1 g) s0 ω1 P(x) ω2 P(A) MGU {x/A} So, let's do a few more examples together, and then you can do some as recitation problems. So, what’s a most general unifier of P(x) and P(A)? A for x. Lecture 7 • 61 61 Most General Unifier g is a most general unifier of ω1 and ω2 iff for all unifiers s...
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y have to be the same as well (to make the middle argument match), they all have to be the same variable. Might as well make it x (though it could be any other variable). 63 Most General Unifier g is a most general unifier of ω1 and ω2 iff for all unifiers s, there exists s0 and ω2 s = (ω2 g) s0 such that ω1...
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)) and G(u). How can we make that work? By substituting F(v) in for u. Lecture 7 • 65 65 Most General Unifier g is a most general unifier of ω1 and ω2 iff for all unifiers s, there exists s0 and ω2 s = (ω2 g) s0 such that ω1 s = (ω1 g) s0 ω1 P(x) ω2 P(A) MGU {x/A} P(F(x), y, G(x)) P(F(x), x, G(x)) {y/x} o...
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(v)), G(u)) P(x, x) {x/G(F(v)), u/F(v)} P(x, F(x)) P(x, x) No MGU! Lecture 7 • 67 The last time I explained this to a class, someone asked me what would happen if F were the identity function. Then, couldn’t we unify these two expressions? That’s a great question, and it illustrates a point I should have made befo...
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we go to a special subroutine that’s shown on the next slide. Lecture 7 • 71 71 Unification Algorithm unify(Expr x, Expr y, Subst s){ if s = fail, return fail else if x = y, return s else if x is a variable, return unify-var(x, y, s) else if y is a variable, return unify-var(y, x, s) else if x is a predicate ...
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) else if x is a predicate or function application, if y has the same operator, return unify(args(x), args(y), s) return fail else else ; x and y have to be lists return unify(rest(x), rest(y), unify(first(x), first(y), s)) } Lecture 7 • 75 Finally, (if we get to this case, then x and y have to be lists, or...
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, s) else if x is bound to val in s, return unify-var(var, val, s) Lecture 7 • 78 Similarly, if x is a variable, and it is bound to val in s, then we have to unify var with val in s. (We call unify-var directly, because we know that var is still a var). 78 Unify-var subroutine Substitute in for var and x as lo...
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careful. The last line of this algorithm in the book is incorrect. Lecture 7 • 81 81 Unification Problems For each pair of sentences, give an MGU. Color(Tweety, Yellow) Color(Tweety, Yellow) Color(Hat(John), Blue) R(F(x), B) R(F(y), x) R(F(y), y, x) Loves(x, y) F(G(w), H(w, J(x, y))) F(G(w), H(w, J(x, u)))...
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Massachusetts Institute of Technology Department of Materials Science and Engineering 77 Massachusetts Avenue, Cambridge MA 02139-4307 3.21 Kinetics of Materials—Spring 2006 February 21, 2006 Lecture 4: Interdiffusion. Effects of electical potential, capillarity, and stress on diffusion potential. References 1. ...
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cient numbers of vacancy sources and sinks. However, it is not unusual to find Kirkendall porosity on one side of the interdiffusion zone. • The mobility Mi that relates the diffusive flux of i to its chemical potential gradient is always posi­ tive. Diffusivities are usually positive also, but not always. For instance...
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1.. -2. -"~~i~;e~a~i·- 30 ESL-, MSL4 . I - .. � .e A �F, El- bm-r-0 tj\ -J~(ti, Z o wrr~s 14% -,L kt,1-6 (C§(2 ) . same 'S%;SA Sq Not ~or sl, c ----------- �I �---�--�------ ---- ·- M~ ·--- ;~~ -.­ ^ AS- 4~~~~~~~~~~~~F Yo -. ..------ -. .P.~~~~~~~N~A ''- ~ ~~ŽL. Tt~ zc j ki ~Y­ i o ...
https://ocw.mit.edu/courses/8-322-quantum-theory-ii-spring-2003/3469fc3f8ad9f1562fbc172aaab9efcd_83228HigherMultiple.pdf
~ roASA4 \ex*n Ccmaair-0o-j r 2 A '-T o 44,1pP- re)AL Cof \C>\^ ( e &~ f\ C","\ C. 7\ Lis ( r, 9, >) 9 (\ \ "b ce4 v A. Co e'AT Mt s %,,,4vrr3 '5ene 6r,, \(, (ft, 6) 6 ;vR- Wa,,v~jrC* J pj C(:j ,,m I es rc-t4~za- 1WxhI C2p-k2lc6
https://ocw.mit.edu/courses/8-322-quantum-theory-ii-spring-2003/3469fc3f8ad9f1562fbc172aaab9efcd_83228HigherMultiple.pdf
LECTURE 19 Brauer Groups In this lecture, we present an overview of Brauer groups. Our presentation will be short on proofs, but we will give precise constructions and formulations of claims. For complete proofs, see [Mil13, Ser79, Boy07]. Our motivating question is: “what was all that stuff about Hamiltonian algebras?”...
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have a short exact sequence 0 → Gal(L2/L1) → G2 → G1 → 0, and maps Brcoh(L1/K) = H 2(G1, L× 1 ) → H 2(G2, L× 1 ) → H 2(G2, L× 2 ) = Brcoh(L2/K) since invariance with respect to G2 implies impvariance with respect to G1, and via the embedding L× 2 . This motivates the following definition. 1 (cid:44)→ L× Definition 19.3....
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- algebra with center K. Then the following are equivalent: (1) A is simple, that is, it has no non-trivial 2-sided ideals. (2) A ⊗K L (cid:39) Mn(L) (i.e., an n × n matrix algebra) for some separable extension L/K. (3) A (cid:39) Mn(D) for some central (i.e., with center K) division (i.e., multi- plicative inverses ex...
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B] ∈ Brcsa(K), so Brcsa(K) forms an abelian group. The proof is omitted; showing that A ⊗K B is simple is rather annoying. We note, however, that matrix algebras over K represent the identity element (or “0 equivalence class”) of Brcsa(K). The inverse of A is A, but with opposite multipli- cation (i.e., x · y := yx), w...
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claim, L is very non- unique. Note that, unlike in this case, such an L need not be Galois over K; examples are hard to find, but were discovered in the 1970s. a) and K( In fact, we can take K( √ √ Claim 19.15. An n2-dimensional central division algebra D/K splits over a degree-n extension L/K if and only if K ⊆ L ⊆ D a...
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39) Brcsa(K/L). Note that the cohomological Brauer group is defined only for Galois extensions L/K, whereas the csa Brauer group is defined for all extensions L/K. This gives meaning to the cohomological definition of the Brauer group. We provide the following (incomplete) proof sketch: Proof. For a G-Galois extension L/K...
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the equivalence class of this csa only depends on ϕ, up to coboundaries, and that it splits over L. Moreover, (cid:3) our map (19.1) is a group isomorphism. This is not an especially deep theorem, despite being far from obvious; the complete proof uses a lot of structure theory that is not particularly memorable. We no...
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This gives ϕ(n): the division algebras come from classes in Z/nZ which do not arise from any smaller Z/mZ. Another upshot is the following: Corollary 19.20. Any degree-n2 central division algebra over K contains every degree-n field extension of L. Proof. Any n-torsion class in Br(K) maps to zero in the Brauer group Br(...
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Asymptotic Expansions of Integrals Lecture 12 The Laplace Method We begin with integrals of the form IΩRæ : X b a e?RvΩxæhΩxædx, (8.8) where vΩxæ and hΩxæ are independent of the parameter R. The variable of integration x is real. We shall show how to find the asymptotic form of IΩRæ as R î K. We note that the ...
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�Ræ u 1 X R K ?K e?[2 d[ : Z R . (8.10) In the above, we have made use of the fact that the Gaussian integral XK given in Appendix A of this chapter. ?K e?[2 d[ is equal to Z , as is If one makes a small mistake in an approximation, the answer one gets can be far off the mark. Thus it is often useful to ha...
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MIT OpenCourseWare http://ocw.mit.edu 18.014 Calculus with Theory Fall 2010 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms.
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MIT OpenCourseWare http://ocw.mit.edu 18.102 Introduction to Functional Analysis Spring 2009 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. 8 LECTURE NOTES FOR 18.102, SPRING 2009 Lecture 3. Tuesday, 10 Feb. Recalled the proof from last time that the bounded o...
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through it all you will understand, before we get to it, the main sorts of arguments needed to prove most of the integrability results we will encounter later. Let V be a normed space with norm � · �V . A completion of V is a Banach space B with the following properties:­ (1) There is an injective (1-1)linear map I...
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}. This always gives an absolutely summable series by the triangle inequality: (3.4) � �t1uk + t2u� k� ≤ |t1| �uk� + |t2| k k k � � �u� k�. LECTURE NOTES FOR 18.102, SPRING 2009 9 Within �V (3.5) consider the linear subspace � S = {uk}; � �uk� < ∞, � � uk = 0 of those which converge to 0. As always ...
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– namely the sequence of norms is itself Cauchy but now in R. Moreover, adding an element of S to {uk} does not change the norm of the sequence of partial sums, since the addtional term tends to zero in norm. Thus �b�B is well-defined for each element b ∈ B and �b�B = 0 means exactly that the sequence {uk} used to d...
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0, 0, · · · , is the limit of the norms of the sequence of partial sums and hence is �v�V so �I(v)�B = �v�V and I(v) = 0 therefore implies v = 0 and hence I is also injective. So, we need to check that B is complete, and also that I(V ) is dense. Here is an extended discussion of the difficulty – of course maybe you ...
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some sense – because it is supposed u( k to represent the sum of the bn’s. Now, it would be very nice if we had the estimate n k (3.11) � � n)�V < ∞ �u( k n k since this should allow us to break up the double sum in some nice way so as to get an absolutely summable series out of the whole thing. The trouble is ...
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j Now, ‘resum the series’ defining instead v1 N1 (n) = � k=1 u( k n), vj (n) = Nj � k=Nj−1 n) and do u( k this setting � = 2−n for the nth series. Check that now � � (3.14) � � (n)�V < ∞. �vk Of course, you should also check that bn = {vk series work just as well as the old ones. (n)} + S so that these ...
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102, SPRING 2009 Problem set 2, Due 11AM Tuesday 24 Feb. I was originally going to make this problem set longer, since there is a missing Tuesday. However, I would prefer you to concentrate on getting all four of these questions really right! Problem 2.1 Finish the proof of the completeness of the space B construc...
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Check that this is an absolutely summable series. (2) For which x ∈ [0, 1) does |fk(x)| converge? � k (3) Describe a function on [0, 1) which is shown to be Lebesgue integrable (as defined in Lecture 4) by the existence of this series and compute its Lebesgue integral. (4) Is this function Riemann integrable (th...
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the areas is less than or equal to that of the containing rectangle. (4) Show that if a finite collection of rectangles has union containing a given rectange then the sum of the areas of the rectangles is at least as large of that of the rectangle contained in the union. (5) Prove the extension of the preceeding re...
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a good faith attempt to answer each question. The first four problems concern the ‘little L p’ spaces lp. Note that you have the choice of doing everything for p = 2 or for all 1 ≤ p < ∞. Everyone who handed in a script received full marks. Problem 1.1 Write out a proof (you can steal it from one of many places but ...
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p = 2p max(|a|p i , |bi|p) ≤ 2p(|ai| + |bi|) (3.19) �a + b�p p = |ai + bi|p ≤ 2p(�a�p + �b�p), � where we use the fact that tp is an increasing function of t ≥ 0. j Now, to see that lp is a normed space we need to check that �a�p is indeed a norm. It is non-negative and �a�p = 0 implies ai = 0 for all i which i...
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xp grows faster than xβ. Moreover, it is differentiable and the derivative only vanishes at xp−1 = β, where it must have a global minimum in x > 0. At this point f (x) = 0 so Young’s inequality follows. Now, applying this with α = |ai|/�a�p and β = |bi|/�b�q (assuming both are non-zero) and summing over i gives H¨ol...
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a normed space. i I did not necessarily expect you to go through the proof of Young-H¨older- Minkowksi, but I think you should do so at some point since I will not do it in class. Problem 1.2 The ‘tricky’ part in Problem 1.1 is the triangle inequality. Suppose you knew – meaning I tell you – that for each N ⎛ ⎝ ...
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finite, but arbitrary, N. Problem 1.3 Prove directly that each lp as defined in Problem 1.1 – or just l2 – is complete, i.e. it is a Banach space. At the risk of offending some, let me say that this means showing that each Cauchy sequence converges. The problem here is to find the limit of a given Cauchy sequence. Sho...
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. Since C is complete (n) − ai (m)| ≤ �a(n) − a(m)�p so each of the sequences ai (n) must (3.29) lim ai n→∞ (n) = ai exists for each i = 1, 2, . . . . So, our putative limit is a, the sequence {ai}∞ The boundedness of the norms shows that i=1. (3.30) N � (n)|p ≤ Ap |ai and we can pass to the limit here a...
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of inter­ changing limits. Problem 1.4 Consider the ‘unit sphere’ in lp – where if you want you can set p = 2. This is the set of vectors of length 1 : S = {a ∈ lp; �a�p = 1}. (1) Show that S is closed. (2) Recall the sequential (so not the open covering definition) characterization of compactness of a set in a m...
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the unit sphere cannot be compact whereas in the former it is. Problem 1.5 Show that the norm on any normed space is continuous. Solution:- Right, so I should have put this problem earlier! The triangle inequality shows that for any u, v in a normed space (3.37) �u� ≤ �u − v� + �v�, �v� ≤ �u − v� + �u� which imp...
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18.311:  Principles  of  Applied  Mathematics Lecture  5   Rodolfo  Ros ales Spring  2014 servation  laws  and  pde:   igher  order  (TRANSPORT)  effects  beyond  quasi Time  it  takes  to  reach  R  =  5  cm  [salt  in  water]. Con H Not fl ux appe • • e   be...
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in  a  silo. ow.   xample  of  a  higher  order  transport  effect  is  viscosity:  Forces  proportional   Another  e to  the  flow  velocity  gradient.  REASON:  the  flow  velocity  is  a  macroscopic  "average"   variable.  The  same  phenomena  that ...
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1st  order  (scalar)  quasilinear  equations  by  characteristics.   Examples:  traffic  flow  and  river  waves. Tra ffic  Flow  equations.  Traffic  density,  flow  and  car  velocity.   r  a  co  nea ati ion t a equ par e by  s Linea Do   Sho s  b ork This  w ...
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for  traffi Density  waves  reach  cars  from  ahead. River  waves  move  faster  than  the  flow. c  flow  u  >  c  and  for  river  flows  u  <  c.   Interpret  equation  as  a  statement  about  a  directional  derivative  of  the  solution  in...
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18.311:  Principles  of  Applied  Mathematics Lecture  5   Rodolfo  Ros ales Spring  2014 Scalar the  cor  hyper respo bolic  equations  can  be  r nding  directional  derivati ves.   educed  to  o.d.e.'s  along  the  cur ves  integrating   2           MIT...
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18.782 Introduction to Arithmetic Geometry Lecture #17 Fall 2013 11/05/2013 Throughout this lecture k denotes an algebraically closed field. 17.1 Tangent spaces and hypersurfaces For any polynomial f ∈ k[x1, . . . , xn] and point P = (a1, . . . , an) ∈ An we define the affine linear form fP (x1, . . . , xn) := (P )(xi − ai...
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= 0 yields gP = (cid:88)(cid:0)hi(P )fi,P + hi,P fi(P ) (cid:1) = (cid:88) hi(P )fi,P , i i (1) which is an element of the ideal (f1,P , . . . , fm,P ). Thus I(Tp(V )) = (f1,P , . . . , fm,P ). When considering the tangent space of a variety at a particular point P , we may assume without loss of generality that P = (0...
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I(TP (V )) is precisely the set of linear forms that vanish at every point in Tp(V ), which, by ∨. Moreover, we see from (1) that every linear definition, is the orthogonal complement TP form in I(TP (V )) is a k-linear combination of f1,P . . . , fm,P . The vector space TP (V )⊥ is called the cotangent space of V at P ...
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of generators for I(V ) and P is a smooth point of V if and only if dim TP = dim V . Remark 17.5. For projective varieties V we defined smooth points P as points that are smooth in all (equivalently, any) affine part containing P . One can also define tangent spaces and Jacobian matrices for projective varieties directly u...
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. . , φ(xn) must be algebraically dependent as elements of k(V ). Thus there exists g ∈ k[x2, . . . , xn] such that g(φ(x2), . . . , φ(xn)) = 0. But then φ(g) = 0, so g ∈ ker φ = (f ). ⊆ Pn, then one of its But this is a contradiction, since degx1 g = 0. So dim V = n − 1. If V affine parts Vi is a hypersurface in A , and...
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1) = 0; such an f exists since γ1, . . . , γn+1 are algebraically dependent. We must have ∂f /∂xi = 0 for some xi; if not than we must have char(k) = p > 0 and f = g(x1, . . . , xn+1) = gp(x1, . . . , xn+1) for some g ∈ k[x1, . . . , xn+1], but this is impossible since f is irreducible. It follows that γi is algebraic,...
https://ocw.mit.edu/courses/18-782-introduction-to-arithmetic-geometry-fall-2013/34da4eafb6fbe4d016d08aa7914a4be7_MIT18_782F13_lec17.pdf
of a hypersurface: if k(V ) = k(γ1, . . . , γn+1) with γ1, . . . , γn) algebraically independent, then there exists an irreducible polynomial f in k[x1, . . . , xn+1] for which f (γ1, . . . , γn+1) = 0, and then V is birationally equivalent to the zero locus of f in An+1. Corollary 17.11. For any point P on an affine var...
https://ocw.mit.edu/courses/18-782-introduction-to-arithmetic-geometry-fall-2013/34da4eafb6fbe4d016d08aa7914a4be7_MIT18_782F13_lec17.pdf
k[An]. ⊆ An is an affine variety, then the maximal ideals mP of its coordinate ring k[V ] = k[A ]/I(V ) are in one-to-one corre- n spondence with the maximal ideals MP of k[An] that contain I(V ); these are precisely the maximal ideals MP for which P ∈ V . If V P as a subspace, and the quotient space MP /M 2 If we choose...
https://ocw.mit.edu/courses/18-782-introduction-to-arithmetic-geometry-fall-2013/34da4eafb6fbe4d016d08aa7914a4be7_MIT18_782F13_lec17.pdf
surjective linear transformation d : MP → TP (V )∨ whose kernel we claim is equal to M 2 P + I(V ) (this is a sum of ideals in k[x1, . . . , xn] that is clearly a subset of MP ). A polynomial f ∈ MP lies in ker d if and only if the restriction of fP to TP (V ) is the zero function, which occurs if and only if fP = gP f...
https://ocw.mit.edu/courses/18-782-introduction-to-arithmetic-geometry-fall-2013/34da4eafb6fbe4d016d08aa7914a4be7_MIT18_782F13_lec17.pdf