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