Paper VII visual guide · Visual 13 of 40 · THE CANONICAL PACKET CONNECTION

Differentiate the subspace itself

Traditional edition: Theorem II.6.1, Theorem II.6.2.

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Continue with \(P(t)=U(t){\operatorname{diag}}(1,0)U(t)^*\) and \(Q(t)=I-P(t)\). Differentiating \(P^2=P\) gives

\[ \dot P P+P\dot P=\dot P, \qquad P\dot P P=0. \]

The second identity says that the derivative has no component entirely inside the current packet. It moves the subspace relative to its complement.

Three matrices give a projector, its derivative, and its connection.
Original drawing. Read the description below; expand the labels and data for selectable text.

Reading the drawing

Read the matrices from left to right at the same parameter value. The identities below state the tangent condition, skew-adjointness, and the commutator relation retained in the source drawing.

Drawing labels and data 16 labels

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  • \(P(0)\)
Drawing grid 1 · rows top to bottom, columns left to right
Row / columnColumn 1Column 2
Row 1\(1\)\(0\)
Row 2\(0\)\(0\)
  • \(\dot P(0)\)
Drawing grid 2 · rows top to bottom, columns left to right
Row / columnColumn 1Column 2
Row 1\(0\)\(1\)
Row 2\(1\)\(0\)
  • \(C\)
Drawing grid 3 · rows top to bottom, columns left to right
Row / columnColumn 1Column 2
Row 1\(0\)\(-1\)
Row 2\(1\)\(0\)
  • \(P\dot P P=0,\qquad C^*=-C,\qquad[C,P]=\dot P\).

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For this complete pair of packets, define

\[ C=\dot P P+\dot Q Q. \]

Exact calculation yields the constant matrix \(C=J\), with \(C^*=-C\) and \([C,P]=\dot P\). At \(t=0\), the displayed small matrices allow these identities to be checked by direct multiplication.

From two packets to a complete family

For differentiable orthogonal projectors \(P_a\) summing to the identity, the paper constructs

\[ C=\sum_a\dot P_aP_a=\frac12\sum_a[\dot P_a,P_a]. \]

This single connection reproduces the motion of every packet in the family. No basis within a packet is needed for this formula. A basis choice would add internal coordinate data without changing which subspaces are selected.

The completeness of the family matters in deriving skew-Hermiticity and the simultaneous transport identities. Using only one summand of an incomplete list is not automatically the same connection. The example retains both \(P\) and \(Q\) throughout, even when the picture emphasizes only the first line.

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The projector derivative describes motion between subspaces. The canonical connection reconstructs that motion from the complete family without choosing internal packet bases.

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