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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55951 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{4}M_{6}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.6165 | 0.7524 | 0.8195 | [M:[1.1717, 0.7323, 0.8283, 0.83, 0.8283, 1.17, 1.2189], q:[0.415, 0.4133], qb:[0.8527, 0.7567], phi:[0.3906]] | [M:[[-3, -3], [2, 4], [3, 3], [-6, -8], [3, 3], [6, 8], [2, 2]], q:[[-3, -4], [6, 7]], qb:[[1, 0], [0, 1]], phi:[[-1, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }M_{3}$, ${ }M_{5}$, ${ }M_{6}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{7}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{6}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{3}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{2}q_{2}\tilde{q}_{1}$ | ${}$ | -3 | t^2.197 + 2*t^2.485 + t^3.51 + t^3.652 + 2*t^3.657 + t^3.662 + t^3.798 + t^4.394 + 2*t^4.682 + t^4.828 + 3*t^4.97 + t^5.707 + t^5.849 + t^5.853 + 2*t^5.995 - 3*t^6. - t^6.005 + 2*t^6.137 + 3*t^6.142 + t^6.147 + 2*t^6.283 + t^6.591 + 2*t^6.879 + t^7.02 - t^7.03 + t^7.162 + 3*t^7.167 - 2*t^7.172 - t^7.177 + t^7.303 + 2*t^7.308 + 2*t^7.313 + t^7.323 + t^7.45 + 5*t^7.455 + t^7.596 + t^7.904 + t^8.045 + t^8.05 + 2*t^8.192 - 3*t^8.197 - t^8.202 + 2*t^8.333 + t^8.338 - t^8.343 + 3*t^8.48 - 6*t^8.485 - 2*t^8.49 + 3*t^8.622 + 4*t^8.627 + 3*t^8.768 + t^8.787 - t^4.172/y - t^6.369/y - t^6.657/y + (2*t^7.682)/y + t^7.687/y + t^7.97/y + t^7.975/y - t^8.565/y + t^8.707/y + t^8.849/y + t^8.853/y + t^8.858/y + (3*t^8.995)/y - t^4.172*y - t^6.369*y - t^6.657*y + 2*t^7.682*y + t^7.687*y + t^7.97*y + t^7.975*y - t^8.565*y + t^8.707*y + t^8.849*y + t^8.853*y + t^8.858*y + 3*t^8.995*y | g1^2*g2^4*t^2.197 + 2*g1^3*g2^3*t^2.485 + g1^6*g2^8*t^3.51 + g1^11*g2^13*t^3.652 + 2*g1^2*g2^2*t^3.657 + t^3.662/(g1^7*g2^9) + g1^7*g2^7*t^3.798 + g1^4*g2^8*t^4.394 + 2*g1^5*g2^7*t^4.682 + g1*g2*t^4.828 + 3*g1^6*g2^6*t^4.97 + g1^8*g2^12*t^5.707 + g1^13*g2^17*t^5.849 + g1^4*g2^6*t^5.853 + 2*g1^9*g2^11*t^5.995 - 3*t^6. - t^6.005/(g1^9*g2^11) + 2*g1^14*g2^16*t^6.137 + 3*g1^5*g2^5*t^6.142 + t^6.147/(g1^4*g2^6) + 2*g1^10*g2^10*t^6.283 + g1^6*g2^12*t^6.591 + 2*g1^7*g2^11*t^6.879 + g1^12*g2^16*t^7.02 - t^7.03/(g1^6*g2^6) + g1^17*g2^21*t^7.162 + 3*g1^8*g2^10*t^7.167 - (2*t^7.172)/(g1*g2) - t^7.177/(g1^10*g2^12) + g1^22*g2^26*t^7.303 + 2*g1^13*g2^15*t^7.308 + 2*g1^4*g2^4*t^7.313 + t^7.323/(g1^14*g2^18) + g1^18*g2^20*t^7.45 + 5*g1^9*g2^9*t^7.455 + g1^14*g2^14*t^7.596 + g1^10*g2^16*t^7.904 + g1^15*g2^21*t^8.045 + g1^6*g2^10*t^8.05 + 2*g1^11*g2^15*t^8.192 - 3*g1^2*g2^4*t^8.197 - t^8.202/(g1^7*g2^7) + 2*g1^16*g2^20*t^8.333 + g1^7*g2^9*t^8.338 - t^8.343/(g1^2*g2^2) + 3*g1^12*g2^14*t^8.48 - 6*g1^3*g2^3*t^8.485 - (2*t^8.49)/(g1^6*g2^8) + 3*g1^17*g2^19*t^8.622 + 4*g1^8*g2^8*t^8.627 + 3*g1^13*g2^13*t^8.768 + g1^8*g2^16*t^8.787 - t^4.172/(g1*g2*y) - (g1*g2^3*t^6.369)/y - (g1^2*g2^2*t^6.657)/y + (2*g1^5*g2^7*t^7.682)/y + t^7.687/(g1^4*g2^4*y) + (g1^6*g2^6*t^7.97)/y + t^7.975/(g1^3*g2^5*y) - (g1^3*g2^7*t^8.565)/y + (g1^8*g2^12*t^8.707)/y + (g1^13*g2^17*t^8.849)/y + (g1^4*g2^6*t^8.853)/y + t^8.858/(g1^5*g2^5*y) + (3*g1^9*g2^11*t^8.995)/y - (t^4.172*y)/(g1*g2) - g1*g2^3*t^6.369*y - g1^2*g2^2*t^6.657*y + 2*g1^5*g2^7*t^7.682*y + (t^7.687*y)/(g1^4*g2^4) + g1^6*g2^6*t^7.97*y + (t^7.975*y)/(g1^3*g2^5) - g1^3*g2^7*t^8.565*y + g1^8*g2^12*t^8.707*y + g1^13*g2^17*t^8.849*y + g1^4*g2^6*t^8.853*y + (t^8.858*y)/(g1^5*g2^5) + 3*g1^9*g2^11*t^8.995*y |
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 |
---|---|---|---|---|---|---|---|---|---|
48214 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{4}M_{6}$ | 0.6342 | 0.7831 | 0.8099 | [M:[1.1646, 0.7243, 0.8354, 0.8285, 0.8354, 1.1715], q:[0.4143, 0.4211], qb:[0.8614, 0.7504], phi:[0.3882]] | t^2.173 + t^2.329 + 2*t^2.506 + t^3.514 + t^3.65 + t^3.671 + t^3.691 + t^3.848 + t^4.346 + t^4.502 + t^4.658 + 2*t^4.679 + 3*t^4.835 + 3*t^5.012 + t^5.687 + t^5.844 + t^5.864 - 2*t^6. - t^4.165/y - t^4.165*y | detail |