Different effects of alternating electric currents (AC) on biological materials have been observed depending on the frequency used. Extremely low frequencies (less than 1 KHz) produce electro-endocytosis at 500 Hz because of membrane depolarization. Intermediate frequencies coincide with tiny particle alignments and cell rotations (also known as the pearl chain effect), thus leading to the tumor-treating fields at 100–300 KHz. High frequencies (i.e., above several MHz) cause tissue heating to predominate due to the dielectric losses. This study investigates how exposure to a wide range of AC electric field frequencies affects the permeability and viability of hepatocellular carcinoma HEPG2 cells. With two silver/silver chloride electrodes, the cells were exposed to a square pulse with a magnitude of 0.4 V/cm at various frequencies between 1 Hz and 1 MHz. A dielectric properties measurement, flow cytometry analysis, fluorescent microscopy, and a polymerase chain reaction (PCR) gene expression analysis were performed. The results showed that all the exposed groups experienced a great reduction in the normal cells, with a clear increase in necrosis and apoptosis compared to the control group. It was noticed that the anti-tumoral effect of the examined frequency range was maximum at 10 KHz and 100 KHz. The permeability was increased in the groups exposed to frequencies above 1 kHz. The viability and permeability results were correlated to the electric relative permittivity, electric conductivity, and gene expression of cyclins A, B, and E.
Citation: Moataz M. Fahmy, Sohier M. El-Kholey, Seham Elabd, Mamdouh M. Shawki. Effect of changing the alternating electric current frequency on the viability of human liver cancer cell line (HEPG2)[J]. AIMS Biophysics, 2025, 12(1): 1-13. doi: 10.3934/biophy.2025001
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Different effects of alternating electric currents (AC) on biological materials have been observed depending on the frequency used. Extremely low frequencies (less than 1 KHz) produce electro-endocytosis at 500 Hz because of membrane depolarization. Intermediate frequencies coincide with tiny particle alignments and cell rotations (also known as the pearl chain effect), thus leading to the tumor-treating fields at 100–300 KHz. High frequencies (i.e., above several MHz) cause tissue heating to predominate due to the dielectric losses. This study investigates how exposure to a wide range of AC electric field frequencies affects the permeability and viability of hepatocellular carcinoma HEPG2 cells. With two silver/silver chloride electrodes, the cells were exposed to a square pulse with a magnitude of 0.4 V/cm at various frequencies between 1 Hz and 1 MHz. A dielectric properties measurement, flow cytometry analysis, fluorescent microscopy, and a polymerase chain reaction (PCR) gene expression analysis were performed. The results showed that all the exposed groups experienced a great reduction in the normal cells, with a clear increase in necrosis and apoptosis compared to the control group. It was noticed that the anti-tumoral effect of the examined frequency range was maximum at 10 KHz and 100 KHz. The permeability was increased in the groups exposed to frequencies above 1 kHz. The viability and permeability results were correlated to the electric relative permittivity, electric conductivity, and gene expression of cyclins A, B, and E.
The importance and usefulness of tensors that are characterized by multiway arrays for big data sets, has been increasingly recognized in the last decades, as testified by a number of surveys [15,20,14,5,17] and among others. Identifiability property (see [3,10,2,9]), including both exact and generic identifiability, is critical for tensor models in various applications, and widely used in many areas, such as signal processing, statistics, computer science, and so on. For instance, in signal processing, the tensor encodes data from received signals and one needs to decompose the tensor to obtain the transmitted signals. If the uniqueness does not hold, one may not recover the transmitted signals. Therefore, to establish the uniqueness property of appropriate tensor decomposition is not only mathematically interest but also necessary in various real applications. Extensive studies under the framework of algebraic geometry have provided various characteristics involving tensor rank and dimensions to ensure generic identifiability.
In this paper, we consider the model of low multilinear rank tensor decomposition (
Definition 1.1. (see Chapter Ⅲ in [19]) Let
(a1,…,αak+βa′k,…,an)−α(a1,…,ak,…,an)−β(a1,…,a′k,…,an) |
for all
An element of
The elements of
If
Kl⊗Km⊗Kn=Kl×m×n |
through the interpretation of the tensor product of vectors as a tensor via the Segre outer product,
[u1,…,ul]T⊗[v1,…,vm]T⊗[w1,…,wn]T=[uivjwk]l,m,ni,j,k=1. |
Definition 1.2. The Khatria-Rao Product is the "matching columnwise" Segre outer product. Given matrices
A⊙B=[a1⊗b1a2⊗b2⋯aK⊗bK]. |
If
Given standard orthnormal bases
X=I1,…,IN∑i1,…,iN=1ti1⋯iNe(1)i1⊗⋯⊗e(N)iN. |
In older literature, the
The rank of
rank(X)=min{r:X=r∑p=1a(1)p⊗⋯⊗a(N)p}. |
Definition 1.3. The
♭n:KI1×⋯×IN→KIn×(I1…ˆIn…IN) |
defined by
(♭n(X))ij=(X)sn(i,j), |
where
For a tensor
r1=dimspanK{X1∙∙,…,Xl∙∙},r2=dimspanK{X∙1∙,…,X∙m∙},r3=dimspanK{X∙∙1,…,X∙∙n}. |
Here
Xi∙∙=[tijk]m,nj,k=1∈Km×n,X∙j∙=[tijk]l,ni,k=1∈Kl×n,X∙∙k=[tijk]l,mi,j=1∈Kl×m. |
The multilinear rank of
Definition 1.4. (see Definition 11 in [4]) A decomposition of a tensor
X=R∑r=1ar⊗Xr, |
in which the
It is clear that in
Definition 1.5. Let
μK{(KI×R×KJ×K×R):X=R∑r=1ar⊗Xr is not unique for ar∈KI,Xr∈KJ×K}. |
Note that in Definition 1.4, we could require
Definition 1.6. A decomposition of a tensor
X=R∑r=1ar⊗Xr. |
As in Definition 1.4,
The main results of the paper are the following, and their proofs will be given in the following sections:
Theorem 1.7. Assume
spanK{Xj1, …, Xjs}∩Σ≤Ljt(KJ×K)⊂{Xj1, …, Xjs}, 1≤t≤s, |
where
Remark 1. In reasonably small cases, one can use tools from numerical algebraic geometry such as those described in [18,12,13].
Remark 2. A generic
p=b′1⊗c′1+⋯+b′L⊗c′L, |
where
We now establish a simpler condition related to the uniqueness of
Theorem 1.8.
I≥2, J=K≠one of {2L1+L22,2L2+L12,L1,L2}. |
Theorem 1.9.
I≥R, K≥R∑r=1Lr, J≥2max{Li}, (Jmax{Li})≥R,Li+Lj>Lk |
for all
For low multilinear rank decomposition in orthogonal frame, we have the following theorem.
Theorem 1.10. A tensor decomposition of
X=R∑r=1ar⊗Xr, |
as in Definition 1.6 is essentially unique if and only if for any non-identity special orthogonal matrix
rank (εk1X1+⋯+εkRXR)≠L1,…,LR. |
In this paper, we first provide some known and preliminary results related to the tensor decompositions of multilinear rank
Definition 2.1. For a vector space
Proof.
a′r∈spanK{a1,…,aR}. |
Since if not, we have
a′∗r∈span⊥K{a1,…,aR}. |
This implies
⟨X, a′∗r⟩=0=X′r, |
which is a contradiction. Therefore, we have
X=R∑r=1a′r⊗X′r=R∑r=1(R∑j=1αrjar⊗X′j), |
we know that
X′r∈spanK{Xj1,…,Xjs}∩Σ≤Lr(KJ×K). |
But
a1⊗X1+⋯+aR⊗XR=a1⊗X′jt−χ2a1⊗X2−⋯−χRa1⊗XR+a2⊗X2+⋯+aR⊗XR=a1⊗X′jt+(a2−χ2a1)⊗X2+⋯+(aR−χRa1)⊗XR=a1⊗X′jt+a′2⊗X2+⋯+a′R⊗XR. |
So
Example 1. A tensor decomposition of
X=R∑r=1ar⊗Xr, |
as in Definition 1.4 is essentially unique if the singular vectors of
Proof. Assume the contrary that
X′r=χ1X1+⋯+χRXR. |
Let
Ur=(|||ur1ur2⋯urJ|||) |
Vr=(|||vr1vr2⋯vrK|||) |
and
Xr=σr1ur1⊗vr1+⋯+σrLrurLr⊗vrLr, |
then we can see the rank of
Proof. It is sufficient to prove the case
Consider
X1=b1,1⊗c1,1+⋯+b1,L1−lb⊗c1,L1−lb+b0,1⊗c1,L1−lb+1+⋯+b0,lb⊗c0,lc∈(B1⊕B0)⊗(C1⊕C0)≅KL1⊗KL1,X2=b2,1⊗c2,1+⋯+b2,L1−lb⊗c2,L1−lb+b0,1⊗c2,L1−lb+1+⋯+b0,lb⊗c0,lc∈(B2⊕B0)⊗(C2⊕C0)≅KL2⊗KL2, |
where
{b0,1,…,b0,lb},{b1,1,…,b1,L1−lb},{b2,1,…,b2,L2−lb},{c0,1,…,c0,lc},{c1,1,…,c1,L1−lc},{c2,1,…,c2,L2−lc}, |
are bases for
(χ1⋱χ1χ1+χ2⋱χ1+χ2χ2⋱χ2) |
has rank
rank (χ1X1+χ2X2)≠L1 or L2 |
if and only if
J,K≠one of {2L1+L22,2L2+L12,L1,L2}. |
Then Theorem 1.8 follows from Theorem 1.7.
Example 2. For
X=a1⊗(b1⊗c1+b2⊗c2)+a2⊗(b2⊗c2+b3⊗c3)=a1⊗(b1⊗c1−b3⊗c3)+(a1+a2)⊗(b2⊗c2+b3⊗c3), |
where
Example 3. For
X=a1⊗(b1⊗c1+b2⊗c2)+a2⊗(b3⊗c1+b4⊗c2)=a1⊗((b1+b3)⊗c1+(b2+b4)⊗c2)+(a2−a1)⊗(b3⊗c1+b4⊗c2), |
where
Example 4. There are explicit Weierstrass canonical forms (see Chapter 10 in [16]) of tensors in
a1⊗(b1⊗c1+⋯+bL⊗cL)+a2⊗(λ1b1⊗c1+⋯+λLbL⊗cL), |
but it is obviously not unique.
Proof. It is sufficient to prove the case
Without loss of generality, for
Ejp=bjp,1⊗cjp,1+bjp,2⊗cjp,2+⋯+bjp,Ljp⊗cjp,Ljp∈Bjp⊗Cjp, |
where
E′jt=b′1⊗c′1+⋯+b′Ljt⊗c′Ljt |
be a general point of
E′jt=∑1≤p≤sχpEjp=∑1≤p≤sχp(bjp,1⊗cjp,1+bjp,2⊗cjp,2+⋯+bjp,Ljp⊗cjp,Ljp). |
If there exist
(xμ⋱xμxμ+xν⋱xμ+xνxν⋱xν) |
has rank at least
The following Remark can be easily obtained using elementary combinatorics.
Remark 3. When
I≥R, J, K≥R∑r=1Lr, Li+Lj>Lk ∀1≤i,j,k≤R, |
a low multilinear rank tensor decomposition of
X=R∑r=1ar⊗[(∑ru=1Lu∑r′=1+∑r−1u=1Lubr′⊗cr′)]. |
Proof.
[X1⋯XR]⊙[e1⋮eR]=[X′1⋯X′R]⊙[e′1⋮e′R]=[X′1⋯X′R]⊙Q[e1⋮eR]. |
Since
X′r=εr1X1+⋯+εrRXR, 1≤r≤R. |
However
rank X′r=rank (εr1X1+⋯+εrRXR)≠L1,…,LR, |
which is a contradiction. Therefore
X′i=εi1X1+⋯+εiRXR, 1≤i≤R, |
we then have
Remark 4. Since the rotation matrix in the plane is
(cos θ−sin θsin θ+cos θ), |
a tensor decomposition of
rank (cosθ X1+sinθ X2)≠L1 or L2, |
and same for
Different from most current approach in the analysis of big data sets, in this paper, some uniqueness characteristics of low multilinear rank tensor decomposition
The first author Ming Yang is grateful to Mingqing Xiao for his insight and for clarity of proofs. The first author is also grateful to the Qiang Cheng's machine learning lab, where this paper was mainly written.
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