Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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56175 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{2}M_{6}$ + ${ }M_{1}^{2}$ + ${ }M_{2}M_{7}$ | 0.7073 | 0.87 | 0.813 | [M:[1.0, 1.041, 0.9181, 0.8771, 1.041, 0.959, 0.959], q:[0.4181, 0.5819], qb:[0.541, 0.541], phi:[0.4795]] | [M:[[0], [2], [-4], [-6], [2], [-2], [-2]], q:[[-4], [4]], qb:[[2], [2]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{4}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{6}^{2}$, ${ }M_{6}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{1}\phi_{1}^{2}$ | ${}M_{4}q_{2}\tilde{q}_{1}$ | -4 | t^2.631 + t^2.754 + 3*t^2.877 + t^3. + t^3.369 + t^3.947 + 2*t^4.316 + t^4.439 + 3*t^4.684 + 2*t^4.807 + t^4.93 + t^5.263 + t^5.385 + 3*t^5.508 + 2*t^5.631 + 7*t^5.754 + t^5.877 - 4*t^6. - t^6.123 + 2*t^6.246 - t^6.369 - t^6.492 + t^6.578 + t^6.701 + t^6.737 + 3*t^6.824 + 2*t^6.947 + 6*t^7.193 + 5*t^7.316 - t^7.439 + 7*t^7.561 + 7*t^7.684 - t^7.807 + 2*t^7.894 - 2*t^7.93 + t^8.017 + 3*t^8.14 + t^8.176 + 4*t^8.263 + t^8.299 + 6*t^8.385 + 2*t^8.508 + 10*t^8.631 - 14*t^8.877 - t^4.439/y - t^7.07/y - t^7.193/y - t^7.316/y + t^7.561/y + t^7.684/y + t^7.807/y + t^8.385/y + (3*t^8.508)/y + (4*t^8.631)/y + (4*t^8.754)/y + (3*t^8.877)/y - t^4.439*y - t^7.07*y - t^7.193*y - t^7.316*y + t^7.561*y + t^7.684*y + t^7.807*y + t^8.385*y + 3*t^8.508*y + 4*t^8.631*y + 4*t^8.754*y + 3*t^8.877*y | t^2.631/g1^6 + t^2.754/g1^4 + (3*t^2.877)/g1^2 + t^3. + g1^6*t^3.369 + t^3.947/g1^9 + (2*t^4.316)/g1^3 + t^4.439/g1 + 3*g1^3*t^4.684 + 2*g1^5*t^4.807 + g1^7*t^4.93 + t^5.263/g1^12 + t^5.385/g1^10 + (3*t^5.508)/g1^8 + (2*t^5.631)/g1^6 + (7*t^5.754)/g1^4 + t^5.877/g1^2 - 4*t^6. - g1^2*t^6.123 + 2*g1^4*t^6.246 - g1^6*t^6.369 - g1^8*t^6.492 + t^6.578/g1^15 + t^6.701/g1^13 + g1^12*t^6.737 + (3*t^6.824)/g1^11 + (2*t^6.947)/g1^9 + (6*t^7.193)/g1^5 + (5*t^7.316)/g1^3 - t^7.439/g1 + 7*g1*t^7.561 + 7*g1^3*t^7.684 - g1^5*t^7.807 + (2*t^7.894)/g1^18 - 2*g1^7*t^7.93 + t^8.017/g1^16 + (3*t^8.14)/g1^14 + g1^11*t^8.176 + (4*t^8.263)/g1^12 + g1^13*t^8.299 + (6*t^8.385)/g1^10 + (2*t^8.508)/g1^8 + (10*t^8.631)/g1^6 - (14*t^8.877)/g1^2 - t^4.439/(g1*y) - t^7.07/(g1^7*y) - t^7.193/(g1^5*y) - t^7.316/(g1^3*y) + (g1*t^7.561)/y + (g1^3*t^7.684)/y + (g1^5*t^7.807)/y + t^8.385/(g1^10*y) + (3*t^8.508)/(g1^8*y) + (4*t^8.631)/(g1^6*y) + (4*t^8.754)/(g1^4*y) + (3*t^8.877)/(g1^2*y) - (t^4.439*y)/g1 - (t^7.07*y)/g1^7 - (t^7.193*y)/g1^5 - (t^7.316*y)/g1^3 + g1*t^7.561*y + g1^3*t^7.684*y + g1^5*t^7.807*y + (t^8.385*y)/g1^10 + (3*t^8.508*y)/g1^8 + (4*t^8.631*y)/g1^6 + (4*t^8.754*y)/g1^4 + (3*t^8.877*y)/g1^2 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
50786 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{2}M_{6}$ + ${ }M_{1}^{2}$ | 0.7037 | 0.8634 | 0.8151 | [M:[1.0, 1.0362, 0.9275, 0.8913, 1.0362, 0.9638], q:[0.4275, 0.5725], qb:[0.5362, 0.5362], phi:[0.4819]] | t^2.674 + t^2.783 + 2*t^2.891 + t^3. + t^3.109 + t^3.326 + t^4.011 + 2*t^4.337 + t^4.446 + 3*t^4.663 + 2*t^4.772 + t^4.88 + t^5.348 + t^5.457 + 2*t^5.565 + t^5.674 + 5*t^5.783 + t^5.891 - 2*t^6. - t^4.446/y - t^4.446*y | detail |