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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48203 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}M_{6}$ | 0.6784 | 0.8213 | 0.826 | [M:[1.0, 0.714, 1.0, 1.0008, 1.1426, 0.9992], q:[0.5004, 0.4996], qb:[0.7857, 0.4996], phi:[0.4287]] | [M:[[-7, 1], [6, 0], [7, -1], [-14, 0], [4, 0], [14, 0]], q:[[-7, 0], [14, -1]], qb:[[1, 0], [0, 1]], phi:[[-2, 0]]] |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }M_{6}$, ${ }M_{3}$, ${ }M_{1}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{5}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{6}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ | ${}M_{1}^{2}$, ${ }M_{3}^{2}$ | -2 | t^2.142 + t^2.998 + 2*t^3. + t^3.428 + 2*t^3.856 + 4*t^4.284 + 2*t^4.286 + t^4.288 + t^5.14 + 2*t^5.142 + t^5.57 + t^5.995 + 2*t^5.998 - 2*t^6. - 2*t^6.002 + 5*t^6.426 + 2*t^6.428 + 2*t^6.853 + 3*t^6.856 - 2*t^6.858 + 4*t^7.281 + 8*t^7.284 + 4*t^7.712 + t^8.137 + 6*t^8.14 - 2*t^8.142 - 2*t^8.144 + 10*t^8.567 + 4*t^8.57 + 2*t^8.572 + 2*t^8.574 + t^8.577 + t^8.993 + 2*t^8.995 - 2*t^8.998 - t^4.286/y - t^6.428/y + t^8.14/y + (2*t^8.142)/y + t^8.144/y + (4*t^8.998)/y - t^4.286*y - t^6.428*y + t^8.14*y + 2*t^8.142*y + t^8.144*y + 4*t^8.998*y | g1^6*t^2.142 + g1^14*t^2.998 + (g1^7*t^3.)/g2 + (g2*t^3.)/g1^7 + g1^4*t^3.428 + (g1^15*t^3.856)/g2 + g1*g2*t^3.856 + 2*g1^12*t^4.284 + (g1^26*t^4.284)/g2^2 + (g2^2*t^4.284)/g1^2 + (g1^5*t^4.286)/g2 + (g2*t^4.286)/g1^9 + t^4.288/g1^16 + g1^20*t^5.14 + (g1^13*t^5.142)/g2 + (g2*t^5.142)/g1 + g1^10*t^5.57 + g1^28*t^5.995 + (g1^21*t^5.998)/g2 + g1^7*g2*t^5.998 - 2*t^6. - t^6.002/(g1^7*g2) - (g2*t^6.002)/g1^21 + 3*g1^18*t^6.426 + (g1^32*t^6.426)/g2^2 + g1^4*g2^2*t^6.426 + (g1^11*t^6.428)/g2 + (g2*t^6.428)/g1^3 + (g1^29*t^6.853)/g2 + g1^15*g2*t^6.853 + g1^8*t^6.856 + (g1^22*t^6.856)/g2^2 + (g2^2*t^6.856)/g1^6 - (g1*t^6.858)/g2 - (g2*t^6.858)/g1^13 + 2*g1^26*t^7.281 + (g1^40*t^7.281)/g2^2 + g1^12*g2^2*t^7.281 + (g1^33*t^7.284)/g2^3 + (3*g1^19*t^7.284)/g2 + 3*g1^5*g2*t^7.284 + (g2^3*t^7.284)/g1^9 + 2*g1^16*t^7.712 + (g1^30*t^7.712)/g2^2 + g1^2*g2^2*t^7.712 + g1^34*t^8.137 + (g1^41*t^8.14)/g2^3 + (2*g1^27*t^8.14)/g2 + 2*g1^13*g2*t^8.14 + (g2^3*t^8.14)/g1 - 2*g1^6*t^8.142 - t^8.144/(g1*g2) - (g2*t^8.144)/g1^15 + 4*g1^24*t^8.567 + (g1^52*t^8.567)/g2^4 + (2*g1^38*t^8.567)/g2^2 + 2*g1^10*g2^2*t^8.567 + (g2^4*t^8.567)/g1^4 + (g1^31*t^8.57)/g2^3 + (g1^17*t^8.57)/g2 + g1^3*g2*t^8.57 + (g2^3*t^8.57)/g1^11 + (g1^10*t^8.572)/g2^2 + (g2^2*t^8.572)/g1^18 + t^8.574/(g1^11*g2) + (g2*t^8.574)/g1^25 + t^8.577/g1^32 + g1^42*t^8.993 + (g1^35*t^8.995)/g2 + g1^21*g2*t^8.995 - 2*g1^14*t^8.998 - t^4.286/(g1^2*y) - (g1^4*t^6.428)/y + (g1^20*t^8.14)/y + (g1^13*t^8.142)/(g2*y) + (g2*t^8.142)/(g1*y) + t^8.144/(g1^8*y) + (2*g1^21*t^8.998)/(g2*y) + (2*g1^7*g2*t^8.998)/y - (t^4.286*y)/g1^2 - g1^4*t^6.428*y + g1^20*t^8.14*y + (g1^13*t^8.142*y)/g2 + (g2*t^8.142*y)/g1 + (t^8.144*y)/g1^8 + (2*g1^21*t^8.998*y)/g2 + 2*g1^7*g2*t^8.998*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 |
---|---|---|---|---|---|---|---|---|---|
46689 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ | 0.6814 | 0.8225 | 0.8284 | [M:[1.0, 0.742, 1.0, 0.9353, 1.1613], q:[0.4677, 0.5323], qb:[0.7903, 0.5323], phi:[0.4193]] | t^2.226 + t^2.806 + 2*t^3. + t^3.484 + 2*t^3.968 + t^4.064 + 2*t^4.258 + 4*t^4.452 + t^5.032 + 2*t^5.226 + t^5.612 + t^5.71 - 2*t^6. - t^4.258/y - t^4.258*y | detail |