Are Lagrangian and Hamiltonian Hessians Always Non-Singular?

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In summary: Conversely, if the Hessian matrix (C) is non-singular, then the Hessian matrix (B) is also non-singular, as can be seen by performing a Legendre transformation on the Hamiltonian.
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espen180
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When going from the Lagrangian to the Hamtiltonian, we define

[tex]p_i=\frac{\partial L}{\partial \dot{q}_i}[/tex]

as the independent variables in place of [tex]\dot{q}[/tex]. This change of variables is possible if and only if the Hessian matrix

[tex]\frac{\partial^2L}{\partial \dot{q}_i\partial\dot{q}_j}[/tex]

is non-singular. The Hamiltonian is then defined by performing a Legendre transformation on the Lagrangian:

[tex]H(q,p,t)\equiv \sum_{i=1}^n \dot{q}_i p_i - L(q,\dot{q},t)[/tex].

Since the first Hamilton's equation is

[tex]\dot{q}_i=\frac{\partial H}{\partial p_i}[/tex]

, this implies that we can perform the inverse change of coordinates if and only if the Hessian matrix

[tex]\frac{\partial^2 H}{\partial p_i \partial p_j}[/tex]

is non-singluar, and we would re-obtain [tex]L[/tex] as

[tex]L(q,\dot{q},t)\equiv \sum_{i=1}^n p_i \dot{q}_i - H(q,p,t)[/tex]

Now for my questions.

1) Does there exist a physical system with a Lagrangian for which [tex]\frac{\partial^2L}{\partial \dot{q}_i\partial\dot{q}_j}[/tex] is singular, or a physical system with a Hamiltonian such that [tex]\frac{\partial^2 H}{\partial p_i \partial p_j}[/tex] is singular?

2) Does the non-singularity of [tex]\frac{\partial^2L}{\partial \dot{q}_i\partial\dot{q}_j}[/tex] immediately imply the non-singularity of [tex]\frac{\partial^2 H}{\partial p_i \partial p_j}[/tex]? If so, how? How about the opposite case (singular implies singular)? Thanks for any help.
 
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A:1) Yes. Consider the Lagrangian $$L~=~\frac{1}{2}m\dot{q}^2. \tag{A}$$ Then the Hessian matrix is $$\left(\frac{\partial^2 L}{\partial \dot{q}_i\partial\dot{q}_j}\right) ~=~m\delta_{ij}. \tag{B}$$ So the Hessian matrix (B) is singular when $m=0$.2) No. The non-singularity of the Hessian matrix (B) does not immediately imply the non-singularity of the Hessian matrix $$\left(\frac{\partial^2 H}{\partial p_i \partial p_j}\right) ~=~\left(\frac{\partial^2 L}{\partial q_i \partial q_j}\right). \tag{C}$$ Consider again the Lagrangian (A). Then the Hessian matrix (B) is non-singular, but the Hessian matrix (C) is singular.
 

FAQ: Are Lagrangian and Hamiltonian Hessians Always Non-Singular?

What is the difference between Lagrangian and Hamiltonian?

The Lagrangian and Hamiltonian are two different mathematical formulations used to describe the dynamics of a physical system. The main difference between them is that the Lagrangian approach uses generalized coordinates, while the Hamiltonian approach uses generalized momenta.

What is the significance of the Lagrangian and Hamiltonian in physics?

The Lagrangian and Hamiltonian formulations are fundamental concepts in classical mechanics, which is a branch of physics that studies the motion of objects. They provide a mathematical framework for describing the dynamics of a system and can be used to derive the equations of motion for a wide range of physical systems.

How do you calculate the Lagrangian and Hamiltonian of a system?

To calculate the Lagrangian of a system, you first need to determine the kinetic and potential energy of the system. The Lagrangian is then given by the difference between the two. The Hamiltonian can be calculated by taking the Legendre transformation of the Lagrangian with respect to the generalized momenta.

Can the Lagrangian and Hamiltonian be used in quantum mechanics?

While the Lagrangian and Hamiltonian formulations were originally developed for classical mechanics, they have also been successfully applied to quantum mechanics. In quantum mechanics, the Lagrangian and Hamiltonian are used to describe the evolution of a quantum system over time.

What are the advantages of using the Lagrangian and Hamiltonian in physics?

The Lagrangian and Hamiltonian formulations have several advantages in physics. They provide a more elegant and concise way to describe the dynamics of a system compared to traditional Newtonian mechanics. They also allow for a more general and systematic approach to solving complex problems and can be easily extended to include additional forces or constraints in a system.

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