The Gaussian transform is
Therefore
A sufficient weak-scattering regime is kinetic energy much larger than (more intrinsically ).
For , the small- transform scales as . Since contributes near forward scattering, the total Born cross section behaves as , finite exactly for . Coulomb decay gives the familiar divergent forward Rutherford cross section and requires long-range treatment.
Insert the incident plane wave for in the integral. At large , , so the outgoing amplitude is
Thus Born approximation gives the stated differential cross section.
Coherent state evolution gives
The condition from part (d) becomes
Since and , the bound is
. The left side is , so equality holds exactly when .
Using and ,
The displacement operator is unitary, so . By coherent state, , hence .
Rotational invariance gives . Direct calculation gives
Take ; angular-momentum brackets imply , and central symmetry gives . Hence are in involution.
At , , . The differentials of and have independent components in the and transverse position directions when ; supplies an independent radial/momentum component. Thus they are locally independent and the system is Liouville integrable.
The conclusion is Arnold-Liouville theorem: a compact connected regular common level is a three-torus, and nearby action-angle coordinates make the flow linear in the angles.
Hamilton's equations are and . A first integral satisfies . See integrable Hamiltonian system: in three degrees of freedom, integrability requires three independent commuting first integrals.
The fixed points are and . At the origin the eigenvalues are and , so it is a saddle. At either nonzero point the characteristic polynomial is
They are stable nodes for , degenerate nodes at equality, and stable spirals above it.
The stable manifold of the origin is exactly . Write the stable manifold in the unstable direction as . Graph invariance gives
Thus has
The required properties are those of a strict Lyapunov function; the domain of stability is the set of initial states whose forward trajectories converge to the fixed point.
For ,
Thus when , proving that disc lies in the basin. On , (with the tangency points checked from the vector field), so trajectories outside cannot enter the basin through that boundary. Hence the basin is contained in .
On an -sample, each coordinate partition has at most placements, hence all partitions have at most configurations. For each fixed configuration, the sign class from a vector space of dimension has at most patterns. Multiplication gives
For each coordinate, the interval indicators sum to one, so the span of all displayed indicators has dimension at most
Therefore VC dimension of a vector space gives
.
Order the sample points. Each of the cut points can occupy one of at most gaps. Once those gaps are chosen the fixed determine every sign, so
For points , count the distinct vectors ; maximize over samples to get . The shattering coefficient equals exactly when some sample is shattered, and the largest such is .
By Gaussian conditional expectation,
Multiply by , take expectations, and use part (c):
Substitution into part (d) gives
The marginal utility price is
The value function is concave; its tangent at zero lies above its graph. Evaluating that supporting inequality at the utility-indifference displacement gives
, hence .
Differentiate expected utility at the optimum in each portfolio direction:
Rearranging gives the claimed vector identity.

Pinned article: Introduction to the OurBigBook Project

Welcome to the OurBigBook Project! Our goal is to create the perfect publishing platform for STEM subjects, and get university-level students to write the best free STEM tutorials ever.
Everyone is welcome to create an account and play with the site: ourbigbook.com/go/register. We belive that students themselves can write amazing tutorials, but teachers are welcome too. You can write about anything you want, it doesn't have to be STEM or even educational. Silly test content is very welcome and you won't be penalized in any way. Just keep it legal!
We have two killer features:
  1. topics: topics group articles by different users with the same title, e.g. here is the topic for the "Fundamental Theorem of Calculus" ourbigbook.com/go/topic/fundamental-theorem-of-calculus
    Articles of different users are sorted by upvote within each article page. This feature is a bit like:
    • a Wikipedia where each user can have their own version of each article
    • a Q&A website like Stack Overflow, where multiple people can give their views on a given topic, and the best ones are sorted by upvote. Except you don't need to wait for someone to ask first, and any topic goes, no matter how narrow or broad
    This feature makes it possible for readers to find better explanations of any topic created by other writers. And it allows writers to create an explanation in a place that readers might actually find it.
    Figure 1.
    Screenshot of the "Derivative" topic page
    . View it live at: ourbigbook.com/go/topic/derivative
  2. local editing: you can store all your personal knowledge base content locally in a plaintext markup format that can be edited locally and published either:
    This way you can be sure that even if OurBigBook.com were to go down one day (which we have no plans to do as it is quite cheap to host!), your content will still be perfectly readable as a static site.
    Figure 5. . You can also edit articles on the Web editor without installing anything locally.
    Video 3.
    Edit locally and publish demo
    . Source. This shows editing OurBigBook Markup and publishing it using the Visual Studio Code extension.
  3. https://raw.githubusercontent.com/ourbigbook/ourbigbook-media/master/feature/x/hilbert-space-arrow.png
  4. Infinitely deep tables of contents:
    Figure 6.
    Dynamic article tree with infinitely deep table of contents
    .
    Descendant pages can also show up as toplevel e.g.: ourbigbook.com/cirosantilli/chordate-subclade
All our software is open source and hosted at: github.com/ourbigbook/ourbigbook
Further documentation can be found at: docs.ourbigbook.com
Feel free to reach our to us for any help or suggestions: docs.ourbigbook.com/#contact