# The Quaternions and the Spaces S 3,

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1 Chapter 10 The Quaternions and the Spaces S 3, SU(2), SO(3), andrp The Algebra H of Quaternions In this chapter, we discuss the representation of rotations of R 3 and R 4 in terms of quaternions. Such a representation is not only concise and elegant, it also yields a very efficient way of handling composition of rotations. It also tends to be numerically more stable than the representation in terms of orthogonal matrices. 431

2 432 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 The group of rotations SO(2) is isomorphic to the group U(1) of complex numbers e iθ = cosθ + i sin θ of unit length. This follows imediately from the fact that the map ( ) e iθ cos θ sin θ sin θ cos θ is a group isomorphism. Geometrically, observe that U(1) is the unit circle S 1. We can identify the plane R 2 with the complex plane C, letting z = x + iy C represent (x, y) R 2. Then, every plane rotation ρ θ by an angle θ is represented by multiplication by the complex number e iθ U(1), in the sense that for all z,z C, z = ρ θ (z) iff z = e iθ z.

3 10.1. THE ALGEBRA H OF QUATERNIONS 433 In some sense, the quaternions generalize the complex numbers in such a way that rotations of R 3 are represented by multiplication by quaternions of unit length. This is basically true with some twists. For instance, quaternion multiplication is not commutative, and a rotation in SO(3) requires conjugation with a(unit)quaternionforitsrepresentation. Instead of the unit circle S 1,weneedtoconsiderthe sphere S 3 in R 4,andU(1) is replaced by SU(2). Recall that the 3-sphere S 3 is the set of points (x, y, z, t) R 4 such that x 2 + y 2 + z 2 + t 2 =1, and that the real projective space RP 3 is the quotient of S 3 modulo the equivalence relation that identifies antipodal points (where (x, y, z, t) and( x, y, z, t) are antipodal points).

4 434 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 The group SO(3) of rotations of R 3 is intimately related to the 3-sphere S 3 and to the real projective space RP 3. The key to this relationship is the fact that rotations can be represented by quaternions, discovered by Hamilton in Historically, the quaternions were the first instance of a noncommutative field. As we shall see, quaternions represent rotations in R 3 very concisely. It will be convenient to define the quaternions as certain 2 2complexmatrices.

5 10.1. THE ALGEBRA H OF QUATERNIONS 435 We write a complex number z as z = a + ib, where a, b R, andtheconjugate z of z is z = a ib. Let 1, i, j, andk be the following matrices: ( ) = 0 1 ( ) 0 1 j = 1 0 ( ) i 0 i = 0 i ( ) 0 i k =. i 0 Consider the set H of all matrices of the form a1 + bi + cj + dk, where (a, b, c, d) R 4.EverymatrixinH is of the form A = ( ) x y, y x where x = a + ib and y = c + id. ThematricesinH are called quaternions.

6 436 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 The null quaternion is denoted as 0 (or 0, ifconfusions arise). Quaternions of the form bi + cj + dk are called pure quaternions. The set of pure quaternions is denoted as H p. Note that the rows (and columns) of such matrices are vectors in C 2 that are orthogonal with respect to the Hermitian inner product of C 2 given by (x 1,y 1 ).(x 2,y 2 )=x 1 x 2 + y 1 y 2. Furthermore, their norm is xx + yy = a2 + b 2 + c 2 + d 2, and the determinant of A is a 2 + b 2 + c 2 + d 2.

7 10.1. THE ALGEBRA H OF QUATERNIONS 437 It is easily seen that the following famous identities (discovered by Hamilton) hold: i 2 = j 2 = k 2 = ijk = 1 ij = ji = k jk = kj = i ki = ik = j. Using these identities, it can be verified that H is a ring (with multiplicative identity 1) andarealvectorspaceof dimension 4 with basis (1, i, j, k). In fact, H is an associative algebra. For details, see Berger [?], Veblen and Young [?], Dieudonné [?], Bertin [?].

8 438 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 The quaternions H are often defined as the real algebra generated by the four elements 1, i, j, k, andsatisfying the identities just stated above. The problem with such a definition is that it is not obvious that the algebraic structure H actually exists. Arigorousjustificationrequiresthenotionsoffreelygenerated algebra and of quotient of an algebra by an ideal. Our definition in terms of matrices makes the existence of H trivial (but requires showing that the identities hold, which is an easy matter).

9 10.1. THE ALGEBRA H OF QUATERNIONS 439 Given any two quaternions X = a1 + bi + cj + dk and Y = a 1 + b i + c j + d k,itcanbeverifiedthat XY =(aa bb cc dd )1 +(ab + ba + cd dc )i +(ac + ca + db bd )j +(ad + da + bc cb )k. It is worth noting that these formulae were discovered independently by Olinde Rodrigues in 1840, a few years before Hamilton (Veblen and Young [?]). However, Rodrigues was working with a different formalism, homogeneous transformations, and he did not discover the quaternions.

10 440 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 The map from R to H defined such that a a1 is an injection which allows us to view R as a subring R1 (in fact, a field) of H. Similarly, the map from R 3 to H defined such that (b, c, d) bi + cj + dk is an injection which allows us to view R 3 as a subspace of H, infact,thehyperplaneh p. Given a quaternion X = a1 + bi + cj + dk, wedefineits conjugate X as It is easily verified that X = a1 bi cj dk. XX =(a 2 + b 2 + c 2 + d 2 )1. The quantity a 2 + b 2 + c 2 + d 2,alsodenotedasN(X), is called the reduced norm of X.

11 10.1. THE ALGEBRA H OF QUATERNIONS 441 Clearly, X is nonnull iff N(X) 0,inwhichcaseX/N(X) is the multiplicative inverse of X. Thus, H is a noncommutative field. Since X + X =2a1, wealsocall2a the reduced trace of X, andwedenoteitastr(x). AquaternionX is a pure quaternion iff X = X iff Tr(X) =0. Thefollowingidentitiescanbeshown(see Berger [?], Dieudonné [?], Bertin [?]): XY = Y X, Tr(XY )=Tr(YX), N(XY )=N(X)N(Y ), Tr(ZXZ 1 )=Tr(X), whenever Z 0.

12 442 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 If X = bi + cj + dk and Y = b i + c j + d k,arepure quaternions, identifying X and Y with the corresponding vectors in R 3,theinnerproductX Y and the crossproduct X Y make sense, and letting [0,X Y ]denote the quaternion whose first component is 0 and whose last three components are those of X Y,wehavetheremarkable identity XY = (X Y )1 +[0,X Y ]. More generally, given a quaternion X = a1+bi+cj+dk, we can write it as X =[a, (b, c, d)], where a is called the scalar part of X and (b, c, d) the pure part of X.

13 10.1. THE ALGEBRA H OF QUATERNIONS 443 Then, if X =[a, U] andy =[a,u ], it is easily seen that the quaternion product XY can be expressed as XY =[aa U U,aU + a U + U U ]. The above formula for quaternion multiplication allows us to show the following fact. Let Z H, andassumethatzx = XZ for all X H. Then, the pure part of Z is null, i.e., Z = a1 for some a R. Remark :Itiseasytocheckthatforarbitraryquaternions X =[a, U] andy =[a,u ], XY YX =[0, 2(U U )], and that for pure quaternion X, Y H p, 2(X Y )1 = (XY + YX).

14 444 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 Since quaternion multiplication is bilinear, for a given X, the map Y XY is linear, and similarly for a given Y, the map X XY is linear. If the matrix of the first map is L X and the matrix of the second map is R Y,then XY = L X Y = a b c d b a d c c d a b d c b a a b c d and XY = R Y X = a b c d b a d c c d a b d c b a a b cd.

15 10.1. THE ALGEBRA H OF QUATERNIONS 445 Observe that the columns (and the rows) of the above matrices are orthogonal. Thus, when X and Y are unit quaternions, both L X and R Y are orthogonal matrices. Furthermore, it is obvious that L X = L X,thetransposeofL X,andsimilarly R Y = RY. It is easily shown that det(l X )=(a 2 + b 2 + c 2 + d 2 ) 2. This shows that when X is a unit quaternion, L X is a rotation matrix, and similarly when Y is a unit quaternion, R Y is a rotation matrix (see Veblen and Young [?]). Define the map ϕ: H H R as follows: ϕ(x, Y )= 1 2 Tr(X Y )=aa + bb + cc + dd.

16 446 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 It is easily verified that ϕ is bilinear, symmetric, and definite positive. Thus, the quaternions form a Euclidean space under the inner product defined by ϕ (see Berger [?], Dieudonné [?], Bertin [?]). It is immediate that under this inner product, the norm of a quaternion X is just N(X). It is also immediate that the set of pure quaternions is orthogonal to the space of real quaternions R1. As a Euclidean space, H is isomorphic to E 4. The subspace H p of pure quaternions inherits a Euclidean structure, and this subspace is isomorphic to the Euclidean space E 3.

17 10.1. THE ALGEBRA H OF QUATERNIONS 447 Since H and E 4 are isomorphic Euclidean spaces, their groups of rotations SO(H) andso(4) are isomorphic, and we will identify them. Similarly, we will identify SO(H p )andso(3).

18 448 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP Quaternions and Rotations in SO(3) We just observed that for any nonnull quaternion X,both maps Y XY and Y YX(where Y H)arelinear maps, and that when N(X) =1,theselinearmapsare in SO(4). This suggests looking at maps ρ Y,Z : H H of the form X YXZ,whereY,Z H are any two fixed nonnull quaternions such that N(Y )N(Z) =1. In view of the identity N(UV) = N(U)N(V )forall U, V H, weseethatρ Y,Z is an isometry.

19 10.2. QUATERNIONS AND ROTATIONS IN SO(3) 449 In fact, since ρ Y,Z = ρ Y,1 ρ 1,Z, ρ Y,Z itself is a rotation, i.e. ρ Y,Z SO(4). We will prove that every rotation in SO(4) arises in this fashion. Also, observe that when Z = Y 1,themapρ Y,Y 1, denoted more simply as ρ Y,istheidentityon1R, andmaps H p into itself. Thus, ρ Z SO(3), i.e., ρ Z is a rotation of E 3. We will prove that every rotation in SO(3) arises in this fashion. The quaternions of norm 1, also called unit quaternions, are in bijection with points of the real 3-sphere S 3.

20 450 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 It is easy to verify that the unit quaternions form a subgroup of the multiplicative group H of nonnull quaternions. In terms of complex matrices, the unit quaternions correspond to the group of unitary complex 2 2matrices of determinant 1 (i.e., xx + yy =1) A = ( ) x y, y x with respect to the Hermitian inner product in C 2. This group is denoted as SU(2). The obvious bijection between SU(2) and S 3 is in fact a homeomorphism, and it can be used to transfer the group structure on SU(2) to S 3,whichbecomesatopological group isomorphic to the topological group SU(2) of unit quaternions. It should also be noted that the fact that the shere S 3 has a group structure is quite exceptional.

21 10.2. QUATERNIONS AND ROTATIONS IN SO(3) 451 As a matter of fact, the only spheres for which a continuous group structure is definable are S 1 and S 3. One of the most important properties of the quaternions is that they can be used to represent rotations of R 3,as stated in the following lemma. Lemma For every quaternion Z 0,themap ρ Z : X ZXZ 1 (where X H) isarotationinso(h) =SO(4) whose restriction to the space H p of pure quaternions is a rotation in SO(H p )=SO(3). Conversely,everyrotation in SO(3) is of the form ρ Z : X ZXZ 1, for some quaternion Z 0, and for all X H p. Furthermore, if two nonnull quaternions Z and Z represent the same rotation, then Z = λz for some λ 0in R.

22 452 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 As a corollary of ρ YX = ρ Y ρ X, it is easy to show that the map ρ: SU(2) SO(3) defined such that ρ(z) =ρ Z is a surjective and continuous homomorphism whose kernel is {1, 1}. Since SU(2) and S 3 are homeomorphic as topological spaces, this shows that SO(3) is homeomorphic to the quotient of the sphere S 3 modulo the antipodal map. But the real projective space RP 3 is defined precisely this way in terms of the antipodal map π: S 3 RP 3,and thus SO(3) and RP 3 are homeomorphic.

23 10.2. QUATERNIONS AND ROTATIONS IN SO(3) 453 This homeomorphism can then be used to transfer the group structure on SO(3) to RP 3 which becomes a topological group. Moreover, it can be shown that SO(3) and RP 3 are diffeomorphic manifolds (see Marsden and Ratiu [?]). Thus, SO(3) and RP 3 are at the same time, groups, topological spaces, and manifolds, and in fact they are Lie groups (see Marsden and Ratiu [?] orbryant[?]). The axis and the angle of a rotation can also be extracted from a quaternion representing that rotation.

24 454 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 Lemma For every quaternion Z = a1+t where t is a nonnull pure quaternion, the axis of the rotation ρ Z associated with Z is determined by the vector in R 3 corresponding to t, andtheangleofrotationθ is equal to π when a =0,orwhena 0,givenasuitable orientation of the plane orthogonal to the axis of rotation, by tan θ N(t) 2 =, a with 0 <θ π. We can write the unit quaternion Z as Z = [cos θ2, sin θ2 ] V, where V is the unit vector t (with π θ π). N(t)

25 10.2. QUATERNIONS AND ROTATIONS IN SO(3) 455 Also note that VV = 1, andthus,formally,everyunit quaternion looks like a complex number cos ϕ + i sin ϕ, except that i is replaced by a unit vector, and multiplication is quaternion multiplication. In order to explain the homomorphism ρ: SU(2) SO(3) more concretely, we now derive the formula for the rotation matrix of a rotation ρ whose axis D is determined by the nonnull vector w and whose angle of rotation is θ. For simplicity, we may assume that w is a unit vector. Letting W =(b, c, d) bethecolumnvectorrepresenting w and H be the plane orthogonal to w, recallthatthe matrices representing the projections p D and p H are WW and I WW.

26 456 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 Given any vector u R 3,thevectorρ(u) canbeexpressed in terms of the vectors p D (u), p H (u), and w p H (u), as ρ(u) =p D (u)+cosθp H (u)+sinθw p H (u). However, it is obvious that so that w p H (u) =w u, ρ(u) =p D (u)+cosθp H (u)+sinθw u, and we know from Section 5.9 that the cross-product w u can be expressed in terms of the multiplication on the left by the matrix A = 0 d c d 0 b. c b 0

27 10.2. QUATERNIONS AND ROTATIONS IN SO(3) 457 Then, letting B = WW = b2 bc bd bc c 2 cd bd cd d 2 the matrix R representing the rotation ρ is, R = WW +cosθ(i WW )+sinθa, =cosθi+sinθa +(1 cos θ)ww, =cosθi+sinθa +(1 cos θ)b. Thus, R =cosθi+sinθa +(1 cos θ)b. with A = 0 d c d 0 b. c b 0

28 458 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 It is immediately verified that A 2 = B I, and thus, R is also given by R = I +sinθa +(1 cos θ)a 2, with A = 0 d c d 0 b. c b 0

29 10.2. QUATERNIONS AND ROTATIONS IN SO(3) 459 Then, the nonnull unit quaternion Z = [cos θ2, sin θ2 ] V, where V =(b, c, d) isaunitvector,correspondstothe rotation ρ Z of matrix R = I +sinθa +(1 cos θ)a 2. with A = 0 d c d 0 b. c b 0

30 460 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 Remark :ArelatedformulaknownasRodrigues formula (1840) gives an expression for a rotation matrix in terms of the exponential of a matrix (the exponential map). Indeed, given (b, c, d) R 3,lettingθ = b 2 + c 2 + d 2, we have e A =cosθi+ sin θ (1 cos θ) A + B, θ θ 2 with A and B as above, but (b, c, d)notnecessarilyaunit vector. We will study exponential maps later on.

31 10.2. QUATERNIONS AND ROTATIONS IN SO(3) 461 Using the matrices L X and R Y introduced earlier, since XY = L X Y = R Y X,fromY = ZXZ 1 = ZXZ/N(Z), we get Y = 1 N(Z) L ZR Z X. Thus, if we want to see the effect of the rotation specified by the quaternion Z in terms of matrices, we simply have to compute the matrix 1 N(Z) L ZR Z = 1 N(Z) a b c d b a d c c d a b d c b a a b c d b a d c c d a b d c b a which yields

32 462 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 1 N(Z) N(Z) a 2 + b 2 c 2 d 2 2bc 2ad 2ac +2bd 0 2bc +2ad a 2 b 2 + c 2 d 2 2ab +2cd 0 2ac +2bd 2ab +2cd a 2 b 2 c 2 + d 2 where N(Z) =a 2 + b 2 + c 2 + d 2. But since every pure quaternion X is a vector whose first component is 0, we see that the rotation matrix R(Z) associated with the quaternion Z is R(Z) = 1 N(Z) ( a 2 + b 2 c 2 d 2 2bc 2ad 2ac +2bd 2bc +2ad a 2 b 2 + c 2 d 2 2ab +2cd 2ac +2bd 2ab +2cd a 2 b 2 c 2 + d 2 ) This expression for a rotation matrix is due to Euler (see Veblen and Young [?]).

33 10.2. QUATERNIONS AND ROTATIONS IN SO(3) 463 It is remarkable that this matrix only contains quadratic polynomials in a, b, c, d. This makes it possible to compute easily a quaternion from a rotation matrix. From a computational point of view, it is worth noting that computing the composition of two rotations ρ Y and ρ Z specified by two quaternions Y,Z using quaternion multiplication (i.e. ρ Y ρ Z = ρ YZ )ischeaperthanusing rotation matrices and matrix multiplication. On the other hand, computing the image of a point X under a rotation ρ Z is more expensive in terms of quaternions (it requires computing ZXZ 1 )thanitisinterms of rotation matrices (where only AX needs to be computed, where A is a rotation matrix). Thus, if many points need to be rotated and the rotation is specified by a quaternion, it is advantageous to precompute the Euler matrix.

34 464 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP Quaternions and Rotations in SO(4) For every nonnull quaternion Z, themapx ZXZ 1 (where X is a pure quaternion) defines a rotation of H p, and conversely every rotation of H p is of the above form. What happens if we consider a map of the form X YXZ, where X H, andn(y )N(Z) =1? Remarkably, it turns out that we get all the rotations of H.

35 10.3. QUATERNIONS AND ROTATIONS IN SO(4) 465 Lemma For every pair (Y,Z) of quaternions such that N(Y )N(Z) =1,themap ρ Y,Z : X YXZ (where X H) isarotationinso(h) = SO(4). Conversely, every rotation in SO(4) is of the form ρ Y,Z : X YXZ, for some quaternions Y,Z, suchthat N(Y )N(Z) =1. Furthermore, if two nonnull pairs of quaternions (Y,Z) and (Y,Z ) represent the same rotation, then Y = λy and Z = λ 1 Z, for some λ 0in R. It is easily seen that ρ (Y Y,ZZ ) = ρ Y,Z ρ Y,Z, and as a corollary, it is it easy to show that the map η: S 3 S 3 SO(4) defined such that η(y,z) =ρ Y,Z is a surjective homomorphism whose kernel is {(1, 1), ( 1, 1)}.

36 466 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 We conclude this Section with a mention of the exponential map, since it has applications to quaternion interpolation, which, in turn, has applications to motion interpolation. Observe that the quaternions i, j, k can also be written as ( ) ( ) i i = = i, 0 i 0 1 ( ) ( ) i j = = i, 1 0 i 0 ( ) ( ) 0 i 0 1 k = = i, i so that, if we define the matrices σ 1,σ 2,σ 3 such that σ 1 = ( ) σ 2 = ( 0 i i 0 ) σ 3 = ( ) 1 0, 0 1 we can write Z = a1 + bi + cj + dk = a1 + i(dσ 1 + cσ 2 + bσ 3 ).

37 10.3. QUATERNIONS AND ROTATIONS IN SO(4) 467 The matrices σ 1,σ 2,σ 3 are called the Pauli spin matrices. Note that their traces are null and that they are Hermitian (recall that a complex matrix is Hermitian iff it is equal to the transpose of its conjugate, i.e., A = A). The somewhat unfortunate order reversal of b, c, d has to do with the traditional convention for listing the Pauli matrices. If we let e 0 = a, e 1 = d, e 2 = c and e 3 = b, thenz can be written as Z = e i(e 1 σ 1 + e 2 σ 2 + e 3 σ 3 ), and e 0,e 1,e 2,e 3 are called the Euler parameters of the rotation specified by Z.

38 468 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 If N(Z) =1,thenwecanalsowrite where Z =cos θ i sin θ 2 (βσ 3 + γσ 2 + δσ 1 ), (β,γ,δ)= 1 sin θ 2 (b, c, d). Letting A = βσ 3 + γσ 2 + δσ 1,itcanbeshownthat e iθa =cosθ 1 + i sin θa, where the exponential is the usual exponential of matrices, i.e., for a square n n matrix M, exp(m) =I n + k 1 M k k!. Note that since A is Hermitian of null trace, ia is skew Hermitian of null trace.

39 10.3. QUATERNIONS AND ROTATIONS IN SO(4) 469 The above formula turns out to define the exponential map from the Lie Algebra of SU(2) to SU(2). The Lie algebra of SU(2) is a real vector space having iσ 1, iσ 2, and iσ 3,asabasis. Now, the vector space R 3 is a Lie algebra if we define the Lie bracket on R 3 as the usual cross-product u v of vectors. Then, the Lie algebra of SU(2) is isomorphic to (R 3, ), and the exponential map can be viewed as a map exp: (R 3, ) SU(2) given by the formula exp(θv) = [cos θ2, sin θ2 ] v, for every vector θv, wherev is a unit vector in R 3,and θ R.

40 470 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP Applications of Euclidean Geometry to Motion Interpolation The exponential map can be used for quaternion interpolation. Given two unit quaternions X, Y,suppose we want to find a quaternion Z interpolating between X and Y. We have to clarify what this means. Since SU(2) is topologically the same as the sphere S 3, we define an interpolant of X and Y as a quaternion Z on the great circle (on the sphere S 3 )determinedbythe intersection of S 3 with the (2-)plane defined by the two points X and Y (viewed as points on S 3 )andtheorgin (0, 0, 0, 0). Then, the points (quaternions) on this great circle can be defined by first rotating X and Y so that X goes to 1 and Y goes to X 1 Y,bymultiplying(ontheleft)by X 1.

41 10.4. APPLICATIONS TO MOTION INTERPOLATION 471 Letting X 1 Y =[cosω, sin Ω w], where π <Ω π, thepointsonthegreatcirclefrom 1 to X 1 Y are given by the quaternions where λ R. (X 1 Y ) λ =[cosλω, sin λω w], This is because X 1 Y = exp(2ωw), and since an interpolant between (0, 0, 0) and 2Ωw is 2λΩw in the Lie algebra of SU(2), the corresponding quaternion is indeed exp(2λω) = [cos λω, sin λω w]. We can t justify all this here, but it is indeed correct.

42 472 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3 If Ω π, then the shortest arc between X and Y is unique, and it corresponds to those λ such that 0 λ 1 (it is a geodesic arc). However, if Ω = π, thenx and Y are antipodal, and there are infinitely many half circles from X to Y. In this case, w can be chosen arbitrarily. Finally, having the arc of great circle between 1 and X 1 Y (assuming Ω π), we get the arc of interpolants Z(λ) between X and Y by performing the inverse rotation from 1 to X and from X 1 Y to Y,i.e.,bymultiplying (on the left) by X, andweget Z(λ) =X(X 1 Y ) λ.

43 10.4. APPLICATIONS TO MOTION INTERPOLATION 473 It is remarkable that a closed-form formula for Z(λ) can be given, as shown by Shoemake [?,?]. If X =[cosθ, sin θu], and Y =[cosϕ, sin ϕv](whereu and v are unit vectors in R 3 ), letting cos Ω = cos θ cos ϕ +sinθ sin ϕ (u v) be the inner product of X and Y viewed as vectors in R 4, it is a bit laborious to show that Z(λ) = sin(1 λ)ω sin Ω X + sin λω sin Ω Y.

44 474 CHAPTER 10. THE QUATERNIONS, THE SPACES S 3, SU(2), SO(3), ANDRP 3

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