pan.world
I have a proof of this theorem, but there is not enough space in this margin
Interpretation of frequency shift in FM-AFM (I)
In the Frequency-Modulation mode of AFM, the cantilever keeps harmonically oscillating during measurement. In contrast to optic microscopy or scanning tunneling microscopy, in which the electromagnetic signals are detected directly by detectors, FM-AFM detects the frequency shift of the cantilever's harmonic oscillation when the distance between sample surface and cantilever's tip changes.
Partial differential equations
Partial differential equations provide information about the relationship between the variables instead of the specific form of the solution function. Determining the specific form of solution needs other constraints such as boundary conditions.
First-order ordinary differential equations
Ordinary differential equations (ODE) are important in physical modeling and deduction.
Vector calculus and spherical average in SAXS
A vector is typically regarded as a geometric entity characterized by a magnitude and a direction. Here are some notes about vector calculus and its basic application in small-angle x-ray scattering (SAXS).
Notes about fluorescence correlation spectroscopy formalism
Let's say the concentration of the component \(j\) in the solution is \(C_j(\vec{r}, t)\), which is a scalar function of coordinates \(\vec{r}\) and time \(t\). For a well-mixed solution, the average of concentration over coordinates and time should be a constant \(<C_j(\vec{r}, t)> = \bar{C}_j\). The local concentration \(C_j(\vec{r}, t)\), however, fluctuates with coordinates and time. The amount of local fluctuation is \(\delta C_j(\vec{r}, t) = C_j(\vec{r}, t)-\bar{C}_j\).
Common probability density functions
Probability and statistics are one of the most common terminologies in scientific data interpretations. They provide us ways to find truths and make conclusions from this stochastic and noisy world. These different probability distributions are heavily coupled. In order to apply these distribution properly, we should understand their origin and derivation, which are the main purpose of this post (for continuous distributions).
Common probability mass functions
Probability and statistics are one of the most common terminologies in scientific data interpretations. They provide us ways to find truths and make conclusions from this stochastic and noisy world. These different probability distributions are heavily coupled. In order to apply these distribution properly, we should understand their origin and derivation, which are the main purpose of this post (for discrete distributions).
Generating functions of probability distributions
Probability mass/density distribution have defined generating functions which faciliate the derivation and the understanding of different probability distributions.
Geometric interpretation about Jacobian determinant
In scientific computing, integration by substitution is a very common skill. For example, we measured a series of practical values of a variable (\(x'\)), of which the distribution (\(g(x')\)) was unknown. But we know the theoretic distribution of the variable (\(f(x)\)) and the correction relationship or mapping relationship between theoretic and practical values (\(x=h(x')\)).
Combinations and particle statistics
Permutation
Let's first consider a set of \(n\) objects, which are all different. The number of all possible arrangements (permutations) is
\[ n(n-1) \cdots 1 = n! \]
Generally, if we select \(k (<n)\) objects from \(n\), the number of permuations is
\[ n(n-1)\cdot\cdot\cdot(n-k+1) = \frac{n!}{(n-k)!} = P(n, k) \]