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Lab Courses at the Department of Physics

 

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Advanced Lab Courses

Lab Course Modern Physics and Advanced Physics Lab Course

  • Organisation
  • Regulations
  • Experiments in Modern Physics (B. Sc.)
  • Advanced Physics Experiments (M. Sc.)

General Information

Lab Course Modern Physics (B. Sc.)

The lab course is part of the bachelor's degree programme in Physics and the teaching degree programme in Physics. The prerequisite for participation is the successful participation in the basic lab courses Classical Physics I and II. Registration for additional services (e.g. further experiments to credit for a later Master's degree programme) will only be accepted if approved by the examination committee of the Physics department.

An overview of the experiments offered in the lab course with a brief description can be found under Experiments in Modern Physics (B. Sc). More detailed descriptions, up-to-date information and the regulations in the lab facility is the content of the associated ILIAS page .

Registration for the lab course takes place via the Campus Plus Portal and is possible

  • for the winter semester from September 1 to September 30, and
  • for the summer semester from March 1 to March 31.

 

Dates in the lecture period:

  • Course 1: Monday 14:00 to 19:00
  • Course 2: Wednesday 14:00 to 19:00

 

Advanced Physics Lab Course (M. Sc.)

The Advanced Physics Lab Course is part of the master's degree programme in Physics. An overview of the experiments offered in the lab course with a brief description can be found under Advanced Physics Experiments (Master). More detailed descriptions, up-to-date information and the regulations in the lab facility is the content of the associated ILIAS page.

Registration for the lab course takes place via the Campus Plus Portal and is possible

  • for the winter semester from September 1 to September 30, and
  • for the summer semester from March 1 to March 31.

 

Dates in the lecture period:

  • Course 1: Monday 09:00 to 14:00
  • Course 2: Monday 14:00 to 19:00 (only if one course is not sufficient)

 

Contact

Management:   Priv.-Doz. Dr. Andreas Naber
Phone: +49-721-608-43416
Organisation and Secretariat:   Mrs Carmen Huck
Phone.: +49-721-608-47741
Opening hours:   Mon: 9:00 - 12:00 and 14:00 - 16:00
Wed: 14.00 - 16.00
Thu: 10.00 - 12.00
Address:   Physics "flat building"
Building 30.22; R. F1-24
Engessserstr.7
76131 Karlsruhe, Germany

Regulations

Scope

The number of experiments to be carried out depends on the degree programme:

  • Bachelor Physics: 6 experiments
  • Teaching Physics: 5 experiments
  • Master Physics: 5 experiments

 

Execution and Protocol

 
Preparation

As in the lab courses Classical Physics I and II, a concise written elaboration of the basics must be drawn up for each attempt, which is then the basis of the introductory discussion of the experimental supervisor with the group. The aim is to determine whether the group has the necessary knowledge to carry out the experiment. An insufficient preparation leads to the termination of the experiment, which is then carried out once on a replacement date.

The documents for the preparation are available on the associated ILIAS pages.

 

Protocols

The submission and recognition of the Protocol is done exclusively in electronic form using the learning platform ILIAS. The protocol must be uploaded to ILIAS before the next experiment begins. Mandatory improvements must be uploaded again one week after the supervisor has returned the protocol with comments.

The Protocol should be structured as follows:

  • a) Cover sheet with name of experiment, surname(s), group number and date
  • b) The aim of the experiment, theoretical foundations
  • c) Experimental set-up
  • d) Execution of the experiment
  • e) Evaluation with formulas, error analysis, discussion of the measurement results
  • f) Original measurement log

The derivation of formula or excerpts from the literature are not required. If texts and graphics from textbooks or the Internet are used, this must be sufficiently identified and quoted with reference to the source.

The accepted protocol as well as all pending consultations must be available no later than 2 weeks after the lecture period of the current semester and must be recognised 4 weeks later.

 

Evaluation

Preparation, experimental procedures and protocols are included in the evaluation. Possible evaluations are "(+)", "(0)", "(-)" and "insufficient". In the case of "insufficient" the attempt is not recognised, so that another experiment must be carried out, which can usually take place only in the next semester.

The partial or complete adoption of texts, numbers or graphics from unindicated sources (or from previous elaborations of the same experiment) is considered a fraud attempt. In the experiment concerned, fraud attempts lead to the evaluation "insufficient" .

The necessary achievements to pass the lab course depend on the course of study:

  • Bachelor: 6 recognized experiments, of which no more than two are rated as "(-)".

  • Master's and teaching degree: 5 recognised attempts, of which no more than one is rated as "(-)"

Experiments in Modern Physics (B. Sc.)

The Labs of Modern Physics are organised topically into three areas, which are supervised by the three experimental institutes of the Faculty of Physics: Applied Physics (APH) , Institute of Physics (PHI) and Experimental Particle Physics (ETP). Of the 5 or 6 experiments to be carried out by a group of two students, one or two experiments are awarded from each area. Experiments with the same prefix (e.g. APH-1) are usually combined.

APH-1: Optical Cloaking
This experiment investigates an optical cloaking device that makes objects invisible in a light-scattering environment (such as fog or milk). The cloaking is based on the faster diffusion of light in the cloak compared to the surrounding environment, which causes the light to be deflected around the object.

APH-1: Lattice Vibrations
A chain of sliders coupled with springs on an air cushion path models longitudinal vibrations of the crystal lattice (phonons). From the natural frequencies, the dispersion relation of the monatomic and the diatomic chain can be determined.

APH-2: Quantum Optics
In this experiment, quantum properties of light are investigated. Single photons are generated, detection techniques are illustrated and basic quantum mechanical concepts such as the superposition of states are demonstrated.

APH-2: Atomic Force Microscope
An atomic force microscope is used to examine the surfaces of a self-assembled monolayer (SAM) of silane-alkanes patterned by micro-contact printing and a CD with respect to topography and friction contrast.

APH-3: Laser Resonator
In this experiment, a pre-assembled titanium:sapphire laser is adjusted and put into laser operation. Subsequently, characteristics and application areas of different laser types are worked out on the basis of the spectra. The experiment gives a good insight into the work in an optical laboratory.

APH-3: Optical Tweezers
In optical tweezers, a highly focused laser beam is used to hold and move microscopic dielectric objects. In the experiment, this principle is being investigated on plastic microparticles. In medicine, the method is used for artificial insemination, among other things.

PHI-1: Scanning Tunneling Microscope
The surfaces of highly oriented pyrolytic graphite (HOPG) and evaporated gold films are examined and characterized by a scanning tunnelling microscope at room temperature.

PHI-1: Mass Spectrometer
A quadrupole mass spectrometer is available in a high vacuum chamber. In addition to the measurement of mass spectra of the residual gas in the vacuum chamber, the ionization energy of argon as well as the decomposition enthalpy of calcium carbonate can be determined.

PHI-2: Nuclear Magnetic Resonance
The aim of this experiment is to determine the spin-spin relaxation by nuclear magnetic resonance (NMR) and to investigate the relationship between the spin-spin relaxation time T2, and the effective spin-spin relaxation time. The T2 time for water is measured using the spin-echo method, and the concept of the NMR imaging technique is explained with a simple experiment.

PHI-2: Bloch waves / Quantum Analogs
In this experiment, various sound wave experiments are carried out, which serve as analogous experiments for certain effects of quantum physics. First, a particle-in-a-box is simulated with the help of sound waves in a closed tube. In addition, the band model, a quantum-mechanical description of electronic energy states in an ideal single-crystalline solid, can also be acoustically modelled by a pipe provided with apertures. In particular, the behaviour of particles in a periodic lattice potential and the formation of these band structures are investigated. With the help of the setup, lattices with multi-atomic base and lattices with defects can also be observed.

PHI-3: Hyperfine Structure
The hyperfine line spectrum of thallium is recorded with a piezo-controlled Fabry-Perot interferometer. The hyperfine splitting of 205Tl can be determined from the interference patterns obtained with a CCD camera.

PHI-3: Material Analysis with X-rays (MAX)
Material analysis with X-rays is an important method in research, development and production for determining the composition of materials and products. In this experiment, you will work with a modern X-ray machine and learn about some important basics of material analysis with X-rays (energy resolution, qualitative and quantitative X-ray fluorescence analysis, etc.). The device is approved as a full protection device within the scope of the Radiation Protection Ordinance.

ETP-1: Drift Rate of Electrons in Gases
The diffusion of electrons in a gas resulting in the ionization of gas molecules/atoms by ionizing radiation is an important process in the detection of high-energy radiation, e.g. in a Geiger-Müller counter tube. In this experiment, the average drift velocity of electrons is measured as a function of gas, acceleration voltage and pressure and compared with theoretical expectation values.

ETP-1: Parity Violation in case of β-Decay
In this experiment, an important conservation rate is tested with the simplest means, the parity in the radioactive beta decay (weak interaction). Quanta of polarized bremsstrahlung (braking radiation) are counted via the compton scattering of magnetized iron in a NaJ scintillation detector. If the parity in beta decay is violated, there are different counting rates depending on the magnetization direction of the iron.

ETP-2: The Lifetime of Positronium
In this experiment, the average lifetime of a positron (anti-particle of the electron) is measured in plexiglass. Positrons annihilate with electrons in two gamma quanta detected with scintillation detectors. In the solid, they usually form an atomic-like state with electrons, the positronium, the life of which depends on the direction of the two particles (Ortho and Parapositronium).

ETP-2: The Compton Effect
This experiment investigates the quasi-elastic scattering of gamma quanta of electrons, the compton scattering. An aluminium cylinder and a scintillation detector, which can be moved around the scatterer at different angles, serves as a scattering target. The energy of the scattered gamma quanta and the counting rate are absorbed as a function of scattering angle and compared with theoretical predictions.

ETP-3: Measuring the Angle Correlation of Gamma Radiation
In gamma decays in which two correlated gamma-ray quanta are emitted in a cascade, the angle between the two gamma measures is no longer isotropically distributed. Two scintillation detectors can measure the count rate of correlated gammas from a 60Co source at different angles and determine the anisotropy of the distribution.

ETP-3: Neutron Diffusion
Fast neutrons from an AmBe source in a water tank are slowed down (thermalized) in the water and detected with a BF3 counter tube at different distances. In addition, a Cd sphere can be used to absorb thermal neutrons around the source. From the two measurements, the relaxation length for fast neutrons and the diffusion length for thermal neutrons in water will be determined.

APH-1: Optical Cloaking
APH-3: Optical Tweezers
APH-3: Laser Resonator
 C. Sürgers
Mass Spectrometer
PHI-3: Material Analysis
  C. Sürgers
Hyperfine Structure
ETP-1: Drift Rate of Electrons in Gases
 J. Wolf
ETP-2: Compton Effect
 J. Wolf
ETP-3: Neutron Diffusion

Advanced Physics Experiments (M. Sc.)

The Advanced Physics Labs are organised topically into three areas, which are supervised by the three experimental institutes of the Faculty of Physics: Applied Physics (APH) , Institute of Physics (PHI) and Experimental Particle Physics (ETP). Of the 5 experiments to be carried out by a group of two students, one or two experiments are awarded from each area. Experiments with the same prefix (e.g. APH-1) are usually combined.

APH-1: Hall effect
Conductivity and Hall effect are measured on a germanium crystal and on a two-dimensional gallium arsenide layered structure. From the dependence on temperature, the band gap of germanium and the phonon energy in gallium arsenide can be determined.

APH-1: Quantum Eraser
Light is emitted into a Mach-Zehnder interferometer with the different paths marked by differently oriented linear polarizers. An interference pattern can only be observed if the path information is "erased" by an additional polarizer. In this analogy experiment, a continuous laser is used instead of single photons.

APH-2: Semiconductor Spectroscopy
Reflection and absorption are measured on various semiconductors (CdS, CdSe, GaAs quantum films) as a function of wavelength at different temperatures. From this, film thicknesses, band gap and density of states are determined.

APH-2: Photoresistance
The bandgap of CdS is estimated from the wavelength dependence of the photoconductivity of a CdS layer. The lifetime of the charge carriers is obtained from the dependence of photoconductivity on the frequency of an intensity-modulated exposure.

APH/PHI-3: Fluorescence Correlation Spectroscopy (FCS)
A confocal fluorescence microscope is used to determine the diffusion coefficients and radii of fluorescent micro- and nanoparticles. This is done by autocorrelation analysis of the emitted light signals. In biophysics, the method is used to study proteins, among other things.

PHI-1: Laser Spectroscopy
The main task of this experiment is the investigation of the hyperfine splitting of the D2 line of rubidium atoms in a gas cell. For this purpose, two different spectroscopic methods are performed and compared: absorption spectroscopy and saturation spectroscopy. Spectroscopy can also be used to stabilize a laser on an absolute frequency.

PHI-1: Specific Heat
The temperature dependence of the specific heat C of Dysprosium is determined in the temperature range T = 77 - 300 K. The measurement is carried out with the adiabatic heating method in a liquid-nitrogen cooled cryostat. The behaviour of C(T) shows the magnetic phase transitions in TC =90 K and TN =180 K.

PHI-2: Magneto-Optical Kerr Effect
Magnetic hysteresis curves M(H) of thin magnetic layers and layer systems are recorded with the polar magneto-optical Kerr effect. To this end, linearly polarized red laser light impinges on the magnetized layer. The rotation of the polarization axis of the reflected light beam by the magnetization of the layer is measured as a function of the magnetic field strength.

PHI-2: Low Temperatures
The electrical conductivities of a simple metal (Cu), a superconductor (Nb) and a doped semiconductor (Si:P) are measured in the temperature range T > 4 - 300 K. In addition, the temperature dependence of the critical magnetic field, above which the superconductor is again normally conducting, is determined. For this purpose, a glass cryostat cooled with liquid nitrogen and liquid helium is used.

PHI-3: Quantum Hall Effect
The characteristic steps in the transverse magnetoresistance R(B) due to the quantum Hall effect of a two-dimensional electron gas (GaAlAs heterostructure) are measured in a cryostat cooled with liquid helium in magnetic fields up to B 6 T at T 2 K. The fine structure constant can be determined from the plateau values.

ETP-1: Properties of Silicon Strip Detectors
This experiment consists of two parts. In the first part, the properties of a Si strip detector, similar to the detector type used in the trace detector of CMS (detector at the LHC, CERN), are examined. In the second part, the signatures of different particle types are identified in the original data of the CMS experiment at the LHC.

ETP-1: Properties of Elementary Particles
In this experiment, original data from the CMS experiment at the LHC (CERN) on various physical questions are analysed. In the first step, you will learn about the signatures of different types of particles in the complex detector system. Then parameters of different types of particles are determined with the help of software (python) and further physical quantities are derived from them.

ETP-2: Gamma Coincidence Spectroscopy
With two different detector types (semiconductors and scintillator), coincidences between simultaneous gamma events are investigated in both detectors, which are formed in a gamma cascade during the decay of 60Co. Previously, the detectors are calibrated with various radioactive sources and detector properties, such as the energy resolution, are examined more closely.

ETP-2: Cosmic Myon Background in the KATRIN Experiment
Large scintillation counters were installed at the main spectrometer of the neutrino experiment KATRIN at KIT Campus North, with which traces of cosmic muons can be detected. For muons that cross the large vacuum tank, KATRIN data can search for temporally correlated background events. In addition, the lifetime of stopped muons can be determined.

ETP-3: The Mößbauer Effect
The Mössbauer effect describes the resonance absorption of gamma quanta in a solid. Due to the oscillating movement of the gamma source above the detector with various absorbers, the gamma energy can be minimally changed and the location and width of the absorption peaks can be determined. With this method, for example, the internal magnetic field in iron can be determined by the Seeman effect or the quadruple split in iron compounds.

ETP-3: Properties of Cosmic Myons
This experiment investigates the polarization of cosmic muons from the upper atmosphere. For this purpose, muons are selected via suitable coincidence conditions between scintillation counters, which were stopped in a magnetic field in a copper plate. Based on the precession of the myon spin in the magnetic field and the associated correlated emission direction of the decaying electrons the polarisation of the muons as well as its lifetime can be determined.   

 

APH-1:Quantum Eraser
 G. Guigas
APH-1: Hall Effect
 G. Guigas
APH-2: Semiconductor Spectroscopy
 C. Sürgers
PHI-1: Laser Spektroscopy
 C. Sürgers
PHI-2: Low Temperatures
 C. Sürgers
PHI-3: Quantum Hall Effect
ETP-1: Silicon Strip Detectors
 J. Wolf
ETP-2: Gamma Coincidence Spektroscopy
ETP-3: Mößbauer Effect
last change: 2025-03-06
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