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Nearly cosine series and generalized trigonometric functions

  • Alessandro Curcio EMAIL logo , Giuseppe Dattoli , Emanuele Di Palma , Pierpaolo Natalini und Paolo Emilio Ricci
Veröffentlicht/Copyright: 17. Juni 2025
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Abstract

In this paper, A class of overlooked trigonometric-like functions is explored, along with the relevant applications. We indeed show that Taylor series, resembling that of an ordinary cosine, are representative of wider classes of functions that are naturally suited to problems ranging from molecular to Laser Physics. The article goes through the original motivations of the proposal and studies the relevant properties within the context of an Umbral interpretation. Their use in applications is discussed within the framework of Free Electron Laser theory, Lennard–Jones potentials and Kramers–Kronig causality identities.

MSC 2020: 33-XX; 47-XX; 78-XX

A Kramers–Kronig relations

We have already mentioned the relevance of NTF to physical processes involving the scattering processes involving the propagation of electromagnetic waves in dense media and, generally, in spectroscopy, for the modeling of line shapes. A distinctive feature of the complex amplitudes describing these processes are the causality conditions linking their real and imaginary parts through a Hilbert transform or Kramers-Kronig relations, characterized by the identities reported below [16]:

(A.1)

sin m ω = - 1 π Re [ - + cos m ( ω ) ω - ω 𝑑 ω ] ,
cos m ω = - 1 π Re [ - + sin m ( ω ) ω - ω 𝑑 ω ] .

A plot of nearly sine and cosine functions is given in Figure 6 for different values of m. It seems obvious that the nearly cosine functions resemble absorption line shapes, i.e., they could represent the imaginary part of a dielectric susceptibility, while the nearly sine functions resemble the real part of a dielectric susceptibility, related to the real index of refraction of a dense medium.

Figure 6 
                  Left: 
                        
                           
                              
                                 c
                                 ⁢
                                 o
                                 ⁢
                                 
                                    s
                                    m
                                 
                                 ⁢
                                 
                                    (
                                    x
                                    )
                                 
                              
                           
                           
                           {cos_{m}(x)}
                        
                      for different values of m; Right: 
                        
                           
                              
                                 s
                                 ⁢
                                 i
                                 ⁢
                                 
                                    n
                                    m
                                 
                                 ⁢
                                 
                                    (
                                    x
                                    )
                                 
                              
                           
                           
                           {sin_{m}(x)}
                        
                      for different values of m.
Figure 6 
                  Left: 
                        
                           
                              
                                 c
                                 ⁢
                                 o
                                 ⁢
                                 
                                    s
                                    m
                                 
                                 ⁢
                                 
                                    (
                                    x
                                    )
                                 
                              
                           
                           
                           {cos_{m}(x)}
                        
                      for different values of m; Right: 
                        
                           
                              
                                 s
                                 ⁢
                                 i
                                 ⁢
                                 
                                    n
                                    m
                                 
                                 ⁢
                                 
                                    (
                                    x
                                    )
                                 
                              
                           
                           
                           {sin_{m}(x)}
                        
                      for different values of m.
Figure 6

Left: c o s m ( x ) for different values of m; Right: s i n m ( x ) for different values of m.

The proof of identities (A.1) can easily be achieved by noting that

- 1 π - + c o s m ( ω ) ω - ω 𝑑 ω = - 1 π - + 1 ω - ω 1 1 + ( m χ ^ ω ) 2 ϕ 0 𝑑 ω = 1 i + χ ^ m ω ϕ 0 = χ ^ m ω - i 1 + ( χ ^ m ω ) 2 ϕ 0 .

Realizing that

Re [ χ ^ m ω - i 1 + ( χ ^ m ω ) 2 ϕ 0 ] = sin m ( ω ) ,

we obtain the first of equations (A.1). The second equation is easy to prove, starting from the definition given in equation (2.6).

An analogous result has been obtained in [5], where the umbral treatment of the Gaussian functions has naturally led to the link between the ordinary Gaussian and the Dawson function.

The key element extending the Hilbert transform to these families of functions is a consequence of their UI, realized through a Lorentzian. The functions

l s ( x ) = 1 1 + x 2 ,
l a ( x ) = x 1 + x 2

provide the most elementary example of Hilbert transform.

B Standard deviation of nearly cosine functions

Nearly cosine functions are surely normalizable, the latter given by equation (2.4). However, it is impossible to define a standard deviation for such functions. Indeed, starting from the Lorentzian umbral image in equation (2.2), it is straightforward to see that the integral

- + ω 2 1 + ( χ ^ m ω ) 2 ϕ 0 𝑑 ω

does not converge.

Even though the previous statement sufficient for our purposes, it requires some refinements.

The Lorentzian umbral image has already been exploited to study the umbral properties of Gaussian-like functions. The ordinary Gaussian has indeed been defined as (see [5])

e - x 2 = 1 1 + c ^ x 2 ϕ 0 ,
c ^ α ϕ 0 = 1 Γ ( 1 + α ) .

Accordingly, the second-order moment can be defined as

(B.1) - + x 2 e - x 2 𝑑 x = - + ( x 2 1 + c ^ x 2 ϕ 0 ) 𝑑 x .

The evaluation of the previous integral is as follows:

- + ( x 2 1 + c ^ x 2 ϕ 0 ) 𝑑 x = - + ( x 2 1 + c ^ x 2 ) 𝑑 x ϕ 0 = 0 + e - s [ - x 2 e - s c ^ x 2 𝑑 x ] 𝑑 s ϕ 0 .

Noting that

[ - x 2 e - s c ^ x 2 𝑑 x ] ϕ 0 = π 2 s - 3 2 c ^ - 3 2 ϕ 0 = π 2 s - 3 2 Γ ( - 1 2 ) ,

we finally obtain

- + ( x 2 1 + c ^ x 2 ϕ 0 ) 𝑑 x = π 2 Γ ( - 1 2 ) 0 + e - s s - 1 2 - 1 𝑑 s = π 2 ,

which seems to contradict the previous statement. The subtle point is that the derivation of the integral in equation (B.1) is based on the following assumptions:

  1. the vacuum can be brought outside the integral,

  2. the integration over s and x can be inverted,

which holds for forms of the umbral operator that allow the convergence of the integral under study [11, 5, 2]. This last point deserves further investigation and will be discussed with more details elsewhere.

References

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Received: 2024-12-11
Revised: 2025-02-26
Accepted: 2025-03-14
Published Online: 2025-06-17

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