A magic eye is a simplistic triode tube that was used as a tuning indicator in radio receivers around the time of world-war II. It has a bowl shaped anode coated with a phosphorescent material that produces a green glow when electrons strike on it. This makes possible to measure the curvature of electrons’ trajectory when the tube is placed in a magnetic field. By measuring the radius of curvature, the applied voltage between cathode and anode and the magnetic field, charge-to-mass ratio of the electron can be measured.
This interesting demonstration utilizes a highly evacuated electron diffraction tube to show the wave behavior of electrons. The electrons are emitted by the thermionic emission and accelerated towards target by applying a very high potential (2000-5000 V). The target is a micro meshed nickel grid on which a thin layer of graphite is deposited. The electrons being diffracted through the graphite satisfy the Bragg’s condition and produce an interference pattern consisting of two rings.
This demonstration uses the famous Michelson interferometer which is used either for precise distance measurements or the wavelength of the laser. An assembly of optical components including HeNe laser, mirrors and converging lenses is used. The interference pattern is produced by splitting the beam into two paths using a 50:50 beam splitter. The movable mirror is motor controlled and computer interfaced, a source of changing the path length and produce a interference fringes.
The classroom demonstrations uses a gamma ray source of Co-60 placed inside a lead container. The radiation is detected with a Geiger muller tube, whose data is brought into the computer. A histogram is built up showing a Poisson distribution. The distribution of decay times is readily observable and the statistical nature of the phenomenon could be explained.
Optical tunneling is demonstrated by frustrated total internal reflection.
- A green laser diode (from a laser pointer) falls on a glass prism. The angle of incidence is greater than a critical angle, resulting in light being totally internal reflection.
- There is evanescent light leaking from the prism. But this light is difficult to tap off, unless a second prism is placed really close to the first one.
the second prism is almost conjoined with the first prism using an index matching fluid (Cargille’s BK 7 Matching Liquid).
- The fluid is able to mate the prisms really well, yet it keeps a small gap between the prisms. Light can tunnel across this classically forbidden region and transmit into the second prism. Total internal reflection has been frustrated.
When a magnetic field is applied perpendicular to the direction of flow of charge carriers, in a semiconductor material, charge carriers experience a force in transverse to the direction of applied magnetic field and carriers flow. This effect is known as Hall effect. Being very simple and straight forward phenomena in physics, Hall effect is a fundamental principle in magnetic field sensing and have many practical applications in our daily life. This demonstration shows Hall effect in semiconductor materials and shows how n-type and p-type semiconductors can be identified.
Cadmium selenide (CdSe) quantum dots are chemically synthesized in the diameter ranges of 2 to 6 nm. These colloidal solutions are excited with a blue laser of wavelength 405 nm and the fluorescence emission spectrum is observed using a fiber optic spectrometer. The emission wavelength depends on the sizes of the dots, the wavelength is directly proportional to the size (radius) of the nanoparticle. The demonstration is a beautiful, lucid example of the effect of size on the quantization of energy levels and brings home the idea of the potential well quite neatly.
Here is a Presentation on fluorescence from CdSe quantum dots shown in class on 18 April 2013.
A neon lamp is placed inside a spectral tube holder and the emission spectrum is observed with a fiber optics spectrometer. The spectrum is loaded into a data analysis software. Some peaks are chosen, notably the 633 nm transition seen in HeNe lasers. The linewidths are determined and the lifetime of the excited states are estimated. This is a nice straightforward demonstration of the energy-time uncertainty relationship, generally difficult to understand.