My first blog entry
Hello everybody, and thank you for visiting. I’m excited, because this is my first Blog post ever, and it’s particularly exciting to be blogging for the scanning probe community. I want to welcome you here to the Nanoprobe Network, and to encourage you to be an active participant. That means not just reading and downloading material, but commenting on other entries (including this one!), contributing to the Forum discussions, submitting News or Events announcements, or sharing software or A/V material.Several other research communities have successfully made use of web-based technologies like these to greatly stimulate the discussion and exchange of ideas, a nice example being iMechanica. We take some of our inspiration from these efforts. But we are also inspired by the energy and enthusiasm of researchers in our community, many of whom have voiced a need to efficiently and effectively share information, techniques, software, ideas, and other resources. So we have designed this site to be versatile and powerful, while also being easy to use.We hope you benefit from it, and that you actively participate. This is your site! Enjoy!
Hello Robert, I am enthused by Nanoprobe Network’s modern focus and matter-of-fact approach. I view atomic force microscopy as a technology for making measurements that may be processed to define nanostructural topology. The mathematics of data processing for these nanoscale images has a limit, though, in resolution of identifiable details.
Now the topic of quantum mechanics and the mathematical procedures for analyzing the mass, energy, force, and waves present in a nanometric AFM-imaged volume is ready for innovation. The future of material or molecular science surely lies in development of the wavefunction model of picotechnical and smaller wave, particle, and field parameters.
This approach can define picotopology where an equation for one atom, similar to a Schrodinger wavefunction for a single atom labeled psi (Z), is designed to fulfill the ground rules of physics.
An imaging psi function is capable of defining the sensor tip of an AFM instrument as a 3D picometric volume in terms of atomic surface layers with fields of force and energy extending beyond. When this sort of AFM atomic modeling is refined it will enhance the control of focus achieved by the magnetic field probe element. In AFM data processing algorithms the topological wavefunction model can advance the application of a probe by interactive scanning techniques which use the mathematical data point map to guide tip motion by interpreting detected data points.
One way to build the atomic psi function is the GT integral based on the series expansion differential of nuclear force radiation of gravity, positrons, and other forcons with valid joule values. This model combines the relativistic Lorenz-Einstein transform functions for time, mass, and energy with the workon quantized wave equations for frequency and wavelength. Quantum symmetry numbers are assigned along the series differential for {e=m(c^2)} emission of nuclear mass to force fields to give 3D imagery to the solutions. Psi pulsates by cycles of nuclear force output and absorption at the frequency {Nhu=e/h}, a cyclic integral.
In brief, when the psi’s internal momentum function is rearranged to the photon gain rule and integrated for spacetime boundaries, with gravity the force bonding space to psi, the {gravity-time} limited function gives a set of 26 wavefunctions. Each is the topological function for a type of energy intermedon waveparticle of the 5/2 kT J internal heat capacity energy cloud. Those 26 energy values intersect the sizes of the fundamental physical constants: h, h-bar, delta, nuclear magneton, beta magneton, k, 5/2 k, 3/2 k. The result is a picoyoctometric, 3D, animated interactive video atomic model image.
Images of the h-bar magnetic energy waveparticle of ~175 picoyoctometers are online at http://www.symmecon.com with essays, graphics, discussions, and the complete guide to MAVCAM (molecular or material animated video computer assisted modeling) titled The Crystalon Door. TCD was an unopposed motion of disclosure in U.S. District (NM) Court of 04/02/01 titled The Solution to the Equation of Schrodinger.
I think it’s OK