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A closed rotation loop with no closed lift: the full turn about an axis lifts from to
Statement refuted
In this item, a curve on is called when it is continuous on and its restriction to is ; no endpoint derivatives are required.
For every closed curve with and every with , there exists a lift of with .
Facts & Assumptions
Given: The curve on , where is the identification of The quaternion rotation map : conjugation on the imaginary quaternions, the unit sphere , and quaternion lifts and is the third standard basis vector, and the curve .
, , , and is the identity of (The quaternion rotation map : conjugation on the imaginary quaternions, the unit sphere , and quaternion lifts Definition and Remark).
The globally defined curve is and ; the Pythagorean identity gives , and the quarter-turn values give (The quaternions : real quadruples with componentwise addition and an explicit multiplication formula matching the table on , The derivatives of sine and cosine are cosine and minus sine, Parity and the Pythagorean identity for sine and cosine, Quarter-turn values and shifts by pi/2 and pi, Euclidean maps and diffeomorphisms).
For a path in on an open interval containing the associated path is (Angular-velocity reconstruction from a unit-quaternion path: for the body angular velocity of is clause 2, The product rule for quaternion and matrix curves, multiplicativity of the quaternion norm, and the conjugation formula clause 1).
For a rotation path on an open interval and a prescribed unit quaternion over its initial value the lift is unique; moreover every lift of that path is for any one of them (Existence, uniqueness and sign ambiguity of the quaternion lift of a rotation path clauses 1-2).
Counterexample
is with , so for every ; also and by [L2].
The path is on by [L3] (applied after extending to an open interval around ); and are both the identity of by [L1].
Take and let be a lift of with . On the nondegenerate open interval the hypothesis of [L4] is satisfied by the restriction of , and is a lift with prescribed value at the interior time ; hence it is the unique such lift, and every lift of is by [L4], in particular or . In the first case , contradicting ; in the second case , contradicting . Hence is a closed loop with no closed lift through ; for the same argument applied to , using from [L1], gives the same contradiction, so the statement is refuted for both preimages of the identity.
Remarks
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The loop is the full turn about the axis ; its lift runs from to , a half turn of the quaternion sphere. This is the standard local demonstration that the two-sheeted cover of by is nontrivial along loops; no claim about fundamental groups is made here, and no physical spin interpretation is asserted.
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The counterexample refutes only the displayed closed-lift statement. It does not assert that every closed rotation loop fails to have a closed lift, nor that some lift with a different initial value could not be closed; the statement refuted is the universal closed-lift claim for the prescribed initial value, and it is false already at the full turn.
Depends on
The quaternion rotation map : conjugation on the imaginary quaternions, the unit sphere , and quaternion lifts
The product rule for quaternion and matrix curves, multiplicativity of the quaternion norm, and the conjugation formula
Existence, uniqueness and sign ambiguity of the quaternion lift of a rotation path
Angular-velocity reconstruction from a unit-quaternion path: for the body angular velocity of is
The quaternions : real quadruples with componentwise addition and an explicit multiplication formula matching the table on
The derivatives of sine and cosine are cosine and minus sine
Parity and the Pythagorean identity for sine and cosine
Quarter-turn values and shifts by pi/2 and pi
Euclidean maps and diffeomorphisms
Dependency tree · 2 levels
Sources
- P. Etingof, MIT 18.745 Lie Groups and Lie Algebras I (Fall 2020), Exercise 3.9(ii) and the Dirac belt-trick discussion: the full turn in SO(3) lifts to a path from a unit quaternion to its negative; pi_1(SO(3)) = Z/2, printed page 26
- J. Sola, Quaternion kinematics for the error-state Kalman filter (arXiv:1711.02508), Section 2.4.6: by the time the quaternion vector makes a half turn (theta = pi) the 3D rotation has completed a full turn; R{-q} = R{q}, printed page 24
- N. Trawny and S. I. Roumeliotis, Indirect Kalman Filter for 3D Attitude Estimation (University of Minnesota, TR-2005-002), Section 1.1: the quaternion q and the quaternion -q describe a rotation to the same final coordinate system position, printed page 2