From 6a59b4fd5473fc2c52ce643bde0236269bda550e Mon Sep 17 00:00:00 2001 From: Francesco Massimo Date: Tue, 21 Nov 2023 12:01:22 +0100 Subject: [PATCH] correction --- doc/source/exercises.rst | 4 ++-- 1 file changed, 2 insertions(+), 2 deletions(-) diff --git a/doc/source/exercises.rst b/doc/source/exercises.rst index 3a3a584..11b3051 100644 --- a/doc/source/exercises.rst +++ b/doc/source/exercises.rst @@ -19,7 +19,7 @@ One of the first variables we define in this simulation is the ``lambda0``, i.e. .. _exercise1: .. admonition:: Exercise 1 - Assuming :math:`\lambda_0=0.8 \mu m` (a typical Ti:Sa laser system), what is the value of the critical density :math:`n_c`? + Assuming :math:`\lambda_0=0.8 \mu m` (a Ti:Sa laser system), what is the value of the critical density :math:`n_c`? What is the value of the reference electric field :math:`E_0=(2\pi m_e c^2)/(e\lambda_0)`? @@ -543,7 +543,7 @@ as well as their weight (from which their charge can be computed). With the same simulation of :ref:`Exercise 13 `, use the script `Follow_electron_bunch_evolution.py `_ to see how the bunch has evolved during the simulation (``%run Follow_electron_bunch_evolution.py`` in ``IPython``). The script reads the ``DiagTrackParticles`` output and - then computes some bunch quantities (`rms` size, emittance, energy, energy spread) + then computes some bunch quantities (`rms` size, emittance, energy, divergence) at each available output iteration. Include the resulting image in your answers.