There are no $3$ linearly independent lightlike vectors such that $u+v+w = 0$.












0












$begingroup$


Consider the Lorentz-Minkowski space $E^n_1$, also known as $mathbb{L}^n$. I want to prove that there are not lightlike linearly independent vectors $u, v, w in E^n_1$ such that $u + v + w = 0$. How to do it? I'm still unfamiliar with the intuition behind such space.










share|cite|improve this question











$endgroup$












  • $begingroup$
    Does this space have 2 spacelike and one timelike variables? or what if not?
    $endgroup$
    – coffeemath
    Dec 8 '18 at 1:38










  • $begingroup$
    @coffeemath Those are all hypotheses I have.
    $endgroup$
    – user71487
    Dec 8 '18 at 1:41












  • $begingroup$
    I don't see how this can be true... can't we take one of the vectors from the future light cone, say $vec{u}$, and the other two to be $-frac{1}{2}vec{u}$? Don't we need to say that they are non-coplanar?
    $endgroup$
    – RandomMathGuy
    Dec 8 '18 at 1:41










  • $begingroup$
    @RandomMathGuy The title (but not the body) specifies that the three vectors must be linearly independent.
    $endgroup$
    – Travis
    Dec 8 '18 at 1:44










  • $begingroup$
    @Travis I should learn to read the titles more carefully!
    $endgroup$
    – RandomMathGuy
    Dec 8 '18 at 1:44
















0












$begingroup$


Consider the Lorentz-Minkowski space $E^n_1$, also known as $mathbb{L}^n$. I want to prove that there are not lightlike linearly independent vectors $u, v, w in E^n_1$ such that $u + v + w = 0$. How to do it? I'm still unfamiliar with the intuition behind such space.










share|cite|improve this question











$endgroup$












  • $begingroup$
    Does this space have 2 spacelike and one timelike variables? or what if not?
    $endgroup$
    – coffeemath
    Dec 8 '18 at 1:38










  • $begingroup$
    @coffeemath Those are all hypotheses I have.
    $endgroup$
    – user71487
    Dec 8 '18 at 1:41












  • $begingroup$
    I don't see how this can be true... can't we take one of the vectors from the future light cone, say $vec{u}$, and the other two to be $-frac{1}{2}vec{u}$? Don't we need to say that they are non-coplanar?
    $endgroup$
    – RandomMathGuy
    Dec 8 '18 at 1:41










  • $begingroup$
    @RandomMathGuy The title (but not the body) specifies that the three vectors must be linearly independent.
    $endgroup$
    – Travis
    Dec 8 '18 at 1:44










  • $begingroup$
    @Travis I should learn to read the titles more carefully!
    $endgroup$
    – RandomMathGuy
    Dec 8 '18 at 1:44














0












0








0


1



$begingroup$


Consider the Lorentz-Minkowski space $E^n_1$, also known as $mathbb{L}^n$. I want to prove that there are not lightlike linearly independent vectors $u, v, w in E^n_1$ such that $u + v + w = 0$. How to do it? I'm still unfamiliar with the intuition behind such space.










share|cite|improve this question











$endgroup$




Consider the Lorentz-Minkowski space $E^n_1$, also known as $mathbb{L}^n$. I want to prove that there are not lightlike linearly independent vectors $u, v, w in E^n_1$ such that $u + v + w = 0$. How to do it? I'm still unfamiliar with the intuition behind such space.







linear-algebra semi-riemannian-geometry






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited Dec 8 '18 at 1:45







user71487

















asked Dec 8 '18 at 1:31









user71487user71487

948




948












  • $begingroup$
    Does this space have 2 spacelike and one timelike variables? or what if not?
    $endgroup$
    – coffeemath
    Dec 8 '18 at 1:38










  • $begingroup$
    @coffeemath Those are all hypotheses I have.
    $endgroup$
    – user71487
    Dec 8 '18 at 1:41












  • $begingroup$
    I don't see how this can be true... can't we take one of the vectors from the future light cone, say $vec{u}$, and the other two to be $-frac{1}{2}vec{u}$? Don't we need to say that they are non-coplanar?
    $endgroup$
    – RandomMathGuy
    Dec 8 '18 at 1:41










  • $begingroup$
    @RandomMathGuy The title (but not the body) specifies that the three vectors must be linearly independent.
    $endgroup$
    – Travis
    Dec 8 '18 at 1:44










  • $begingroup$
    @Travis I should learn to read the titles more carefully!
    $endgroup$
    – RandomMathGuy
    Dec 8 '18 at 1:44


















  • $begingroup$
    Does this space have 2 spacelike and one timelike variables? or what if not?
    $endgroup$
    – coffeemath
    Dec 8 '18 at 1:38










  • $begingroup$
    @coffeemath Those are all hypotheses I have.
    $endgroup$
    – user71487
    Dec 8 '18 at 1:41












  • $begingroup$
    I don't see how this can be true... can't we take one of the vectors from the future light cone, say $vec{u}$, and the other two to be $-frac{1}{2}vec{u}$? Don't we need to say that they are non-coplanar?
    $endgroup$
    – RandomMathGuy
    Dec 8 '18 at 1:41










  • $begingroup$
    @RandomMathGuy The title (but not the body) specifies that the three vectors must be linearly independent.
    $endgroup$
    – Travis
    Dec 8 '18 at 1:44










  • $begingroup$
    @Travis I should learn to read the titles more carefully!
    $endgroup$
    – RandomMathGuy
    Dec 8 '18 at 1:44
















$begingroup$
Does this space have 2 spacelike and one timelike variables? or what if not?
$endgroup$
– coffeemath
Dec 8 '18 at 1:38




$begingroup$
Does this space have 2 spacelike and one timelike variables? or what if not?
$endgroup$
– coffeemath
Dec 8 '18 at 1:38












$begingroup$
@coffeemath Those are all hypotheses I have.
$endgroup$
– user71487
Dec 8 '18 at 1:41






$begingroup$
@coffeemath Those are all hypotheses I have.
$endgroup$
– user71487
Dec 8 '18 at 1:41














$begingroup$
I don't see how this can be true... can't we take one of the vectors from the future light cone, say $vec{u}$, and the other two to be $-frac{1}{2}vec{u}$? Don't we need to say that they are non-coplanar?
$endgroup$
– RandomMathGuy
Dec 8 '18 at 1:41




$begingroup$
I don't see how this can be true... can't we take one of the vectors from the future light cone, say $vec{u}$, and the other two to be $-frac{1}{2}vec{u}$? Don't we need to say that they are non-coplanar?
$endgroup$
– RandomMathGuy
Dec 8 '18 at 1:41












$begingroup$
@RandomMathGuy The title (but not the body) specifies that the three vectors must be linearly independent.
$endgroup$
– Travis
Dec 8 '18 at 1:44




$begingroup$
@RandomMathGuy The title (but not the body) specifies that the three vectors must be linearly independent.
$endgroup$
– Travis
Dec 8 '18 at 1:44












$begingroup$
@Travis I should learn to read the titles more carefully!
$endgroup$
– RandomMathGuy
Dec 8 '18 at 1:44




$begingroup$
@Travis I should learn to read the titles more carefully!
$endgroup$
– RandomMathGuy
Dec 8 '18 at 1:44










1 Answer
1






active

oldest

votes


















1












$begingroup$

Hint Suppose there were. Expand $$0 = [{bf u} + {bf v} + {bf w}] cdot [{bf u} - ({bf v} + {bf w})]$$ to conclude that ${bf v} cdot {bf w} = 0$.




Additional hint What is the matrix representation of the bilinear form $cdot$ with respect to the basis $({bf u}, {bf v}, {bf w})$?







share|cite|improve this answer









$endgroup$













  • $begingroup$
    Since I wrote this answer, OP edited the question to address the case of $n$-dimensional Minkowski space $mathbb L^n$ rather than just the special case $n = 3$. The initial hint still leads to a solution for the general case, but of course $({bf u}, {bf v}, {bf w})$ is not a basis of $mathbb L^n$ for $n neq 3$.
    $endgroup$
    – Travis
    Dec 8 '18 at 1:48










  • $begingroup$
    Shouldn't I conclude ${bf u} cdot {bf w} = 0$ instead?
    $endgroup$
    – user71487
    Dec 8 '18 at 1:58










  • $begingroup$
    I don't see how---after all, the expression is symmetric in ${bf v}$ and ${bf w}$.
    $endgroup$
    – Travis
    Dec 8 '18 at 2:02






  • 1




    $begingroup$
    Expanding gives $0 = {bf u} cdot {bf u} - ({bf v} + {bf w}) cdot ({bf v} + {bf w}) = -({bf v} cdot {bf v} + 2 {bf v} cdot {bf w} + {bf w} cdot {bf w}) = -2 {bf v} cdot {bf w}$.
    $endgroup$
    – Travis
    Dec 8 '18 at 2:58






  • 1




    $begingroup$
    Not directly anyway. By symmetry of notation, we also have ${bf u} cdot {bf v} = {bf w} cdot {bf u} = 0$, but for $n = 3$ that means all pairs of basis vectors are orthogonal, which implies that $cdot$ is the zero bilinear form, a contradiction.
    $endgroup$
    – Travis
    Dec 8 '18 at 3:00











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1 Answer
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1 Answer
1






active

oldest

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active

oldest

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active

oldest

votes









1












$begingroup$

Hint Suppose there were. Expand $$0 = [{bf u} + {bf v} + {bf w}] cdot [{bf u} - ({bf v} + {bf w})]$$ to conclude that ${bf v} cdot {bf w} = 0$.




Additional hint What is the matrix representation of the bilinear form $cdot$ with respect to the basis $({bf u}, {bf v}, {bf w})$?







share|cite|improve this answer









$endgroup$













  • $begingroup$
    Since I wrote this answer, OP edited the question to address the case of $n$-dimensional Minkowski space $mathbb L^n$ rather than just the special case $n = 3$. The initial hint still leads to a solution for the general case, but of course $({bf u}, {bf v}, {bf w})$ is not a basis of $mathbb L^n$ for $n neq 3$.
    $endgroup$
    – Travis
    Dec 8 '18 at 1:48










  • $begingroup$
    Shouldn't I conclude ${bf u} cdot {bf w} = 0$ instead?
    $endgroup$
    – user71487
    Dec 8 '18 at 1:58










  • $begingroup$
    I don't see how---after all, the expression is symmetric in ${bf v}$ and ${bf w}$.
    $endgroup$
    – Travis
    Dec 8 '18 at 2:02






  • 1




    $begingroup$
    Expanding gives $0 = {bf u} cdot {bf u} - ({bf v} + {bf w}) cdot ({bf v} + {bf w}) = -({bf v} cdot {bf v} + 2 {bf v} cdot {bf w} + {bf w} cdot {bf w}) = -2 {bf v} cdot {bf w}$.
    $endgroup$
    – Travis
    Dec 8 '18 at 2:58






  • 1




    $begingroup$
    Not directly anyway. By symmetry of notation, we also have ${bf u} cdot {bf v} = {bf w} cdot {bf u} = 0$, but for $n = 3$ that means all pairs of basis vectors are orthogonal, which implies that $cdot$ is the zero bilinear form, a contradiction.
    $endgroup$
    – Travis
    Dec 8 '18 at 3:00
















1












$begingroup$

Hint Suppose there were. Expand $$0 = [{bf u} + {bf v} + {bf w}] cdot [{bf u} - ({bf v} + {bf w})]$$ to conclude that ${bf v} cdot {bf w} = 0$.




Additional hint What is the matrix representation of the bilinear form $cdot$ with respect to the basis $({bf u}, {bf v}, {bf w})$?







share|cite|improve this answer









$endgroup$













  • $begingroup$
    Since I wrote this answer, OP edited the question to address the case of $n$-dimensional Minkowski space $mathbb L^n$ rather than just the special case $n = 3$. The initial hint still leads to a solution for the general case, but of course $({bf u}, {bf v}, {bf w})$ is not a basis of $mathbb L^n$ for $n neq 3$.
    $endgroup$
    – Travis
    Dec 8 '18 at 1:48










  • $begingroup$
    Shouldn't I conclude ${bf u} cdot {bf w} = 0$ instead?
    $endgroup$
    – user71487
    Dec 8 '18 at 1:58










  • $begingroup$
    I don't see how---after all, the expression is symmetric in ${bf v}$ and ${bf w}$.
    $endgroup$
    – Travis
    Dec 8 '18 at 2:02






  • 1




    $begingroup$
    Expanding gives $0 = {bf u} cdot {bf u} - ({bf v} + {bf w}) cdot ({bf v} + {bf w}) = -({bf v} cdot {bf v} + 2 {bf v} cdot {bf w} + {bf w} cdot {bf w}) = -2 {bf v} cdot {bf w}$.
    $endgroup$
    – Travis
    Dec 8 '18 at 2:58






  • 1




    $begingroup$
    Not directly anyway. By symmetry of notation, we also have ${bf u} cdot {bf v} = {bf w} cdot {bf u} = 0$, but for $n = 3$ that means all pairs of basis vectors are orthogonal, which implies that $cdot$ is the zero bilinear form, a contradiction.
    $endgroup$
    – Travis
    Dec 8 '18 at 3:00














1












1








1





$begingroup$

Hint Suppose there were. Expand $$0 = [{bf u} + {bf v} + {bf w}] cdot [{bf u} - ({bf v} + {bf w})]$$ to conclude that ${bf v} cdot {bf w} = 0$.




Additional hint What is the matrix representation of the bilinear form $cdot$ with respect to the basis $({bf u}, {bf v}, {bf w})$?







share|cite|improve this answer









$endgroup$



Hint Suppose there were. Expand $$0 = [{bf u} + {bf v} + {bf w}] cdot [{bf u} - ({bf v} + {bf w})]$$ to conclude that ${bf v} cdot {bf w} = 0$.




Additional hint What is the matrix representation of the bilinear form $cdot$ with respect to the basis $({bf u}, {bf v}, {bf w})$?








share|cite|improve this answer












share|cite|improve this answer



share|cite|improve this answer










answered Dec 8 '18 at 1:43









TravisTravis

59.9k767146




59.9k767146












  • $begingroup$
    Since I wrote this answer, OP edited the question to address the case of $n$-dimensional Minkowski space $mathbb L^n$ rather than just the special case $n = 3$. The initial hint still leads to a solution for the general case, but of course $({bf u}, {bf v}, {bf w})$ is not a basis of $mathbb L^n$ for $n neq 3$.
    $endgroup$
    – Travis
    Dec 8 '18 at 1:48










  • $begingroup$
    Shouldn't I conclude ${bf u} cdot {bf w} = 0$ instead?
    $endgroup$
    – user71487
    Dec 8 '18 at 1:58










  • $begingroup$
    I don't see how---after all, the expression is symmetric in ${bf v}$ and ${bf w}$.
    $endgroup$
    – Travis
    Dec 8 '18 at 2:02






  • 1




    $begingroup$
    Expanding gives $0 = {bf u} cdot {bf u} - ({bf v} + {bf w}) cdot ({bf v} + {bf w}) = -({bf v} cdot {bf v} + 2 {bf v} cdot {bf w} + {bf w} cdot {bf w}) = -2 {bf v} cdot {bf w}$.
    $endgroup$
    – Travis
    Dec 8 '18 at 2:58






  • 1




    $begingroup$
    Not directly anyway. By symmetry of notation, we also have ${bf u} cdot {bf v} = {bf w} cdot {bf u} = 0$, but for $n = 3$ that means all pairs of basis vectors are orthogonal, which implies that $cdot$ is the zero bilinear form, a contradiction.
    $endgroup$
    – Travis
    Dec 8 '18 at 3:00


















  • $begingroup$
    Since I wrote this answer, OP edited the question to address the case of $n$-dimensional Minkowski space $mathbb L^n$ rather than just the special case $n = 3$. The initial hint still leads to a solution for the general case, but of course $({bf u}, {bf v}, {bf w})$ is not a basis of $mathbb L^n$ for $n neq 3$.
    $endgroup$
    – Travis
    Dec 8 '18 at 1:48










  • $begingroup$
    Shouldn't I conclude ${bf u} cdot {bf w} = 0$ instead?
    $endgroup$
    – user71487
    Dec 8 '18 at 1:58










  • $begingroup$
    I don't see how---after all, the expression is symmetric in ${bf v}$ and ${bf w}$.
    $endgroup$
    – Travis
    Dec 8 '18 at 2:02






  • 1




    $begingroup$
    Expanding gives $0 = {bf u} cdot {bf u} - ({bf v} + {bf w}) cdot ({bf v} + {bf w}) = -({bf v} cdot {bf v} + 2 {bf v} cdot {bf w} + {bf w} cdot {bf w}) = -2 {bf v} cdot {bf w}$.
    $endgroup$
    – Travis
    Dec 8 '18 at 2:58






  • 1




    $begingroup$
    Not directly anyway. By symmetry of notation, we also have ${bf u} cdot {bf v} = {bf w} cdot {bf u} = 0$, but for $n = 3$ that means all pairs of basis vectors are orthogonal, which implies that $cdot$ is the zero bilinear form, a contradiction.
    $endgroup$
    – Travis
    Dec 8 '18 at 3:00
















$begingroup$
Since I wrote this answer, OP edited the question to address the case of $n$-dimensional Minkowski space $mathbb L^n$ rather than just the special case $n = 3$. The initial hint still leads to a solution for the general case, but of course $({bf u}, {bf v}, {bf w})$ is not a basis of $mathbb L^n$ for $n neq 3$.
$endgroup$
– Travis
Dec 8 '18 at 1:48




$begingroup$
Since I wrote this answer, OP edited the question to address the case of $n$-dimensional Minkowski space $mathbb L^n$ rather than just the special case $n = 3$. The initial hint still leads to a solution for the general case, but of course $({bf u}, {bf v}, {bf w})$ is not a basis of $mathbb L^n$ for $n neq 3$.
$endgroup$
– Travis
Dec 8 '18 at 1:48












$begingroup$
Shouldn't I conclude ${bf u} cdot {bf w} = 0$ instead?
$endgroup$
– user71487
Dec 8 '18 at 1:58




$begingroup$
Shouldn't I conclude ${bf u} cdot {bf w} = 0$ instead?
$endgroup$
– user71487
Dec 8 '18 at 1:58












$begingroup$
I don't see how---after all, the expression is symmetric in ${bf v}$ and ${bf w}$.
$endgroup$
– Travis
Dec 8 '18 at 2:02




$begingroup$
I don't see how---after all, the expression is symmetric in ${bf v}$ and ${bf w}$.
$endgroup$
– Travis
Dec 8 '18 at 2:02




1




1




$begingroup$
Expanding gives $0 = {bf u} cdot {bf u} - ({bf v} + {bf w}) cdot ({bf v} + {bf w}) = -({bf v} cdot {bf v} + 2 {bf v} cdot {bf w} + {bf w} cdot {bf w}) = -2 {bf v} cdot {bf w}$.
$endgroup$
– Travis
Dec 8 '18 at 2:58




$begingroup$
Expanding gives $0 = {bf u} cdot {bf u} - ({bf v} + {bf w}) cdot ({bf v} + {bf w}) = -({bf v} cdot {bf v} + 2 {bf v} cdot {bf w} + {bf w} cdot {bf w}) = -2 {bf v} cdot {bf w}$.
$endgroup$
– Travis
Dec 8 '18 at 2:58




1




1




$begingroup$
Not directly anyway. By symmetry of notation, we also have ${bf u} cdot {bf v} = {bf w} cdot {bf u} = 0$, but for $n = 3$ that means all pairs of basis vectors are orthogonal, which implies that $cdot$ is the zero bilinear form, a contradiction.
$endgroup$
– Travis
Dec 8 '18 at 3:00




$begingroup$
Not directly anyway. By symmetry of notation, we also have ${bf u} cdot {bf v} = {bf w} cdot {bf u} = 0$, but for $n = 3$ that means all pairs of basis vectors are orthogonal, which implies that $cdot$ is the zero bilinear form, a contradiction.
$endgroup$
– Travis
Dec 8 '18 at 3:00


















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