Landscape




$a$ =

$c$ =

$\leq a \leq$

$\leq c \leq$

id =





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.

#TheorySuperpotentialCentral charge $a$Central charge $c$Ratio $a/c$Matter field: $R$-chargeU(1) part of $F_{UV}$Rank of $F_{UV}$Rational
50964 SU2adj1nf2 $M_1q_1q_2$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ + $ M_2q_2\tilde{q}_1$ + $ M_3q_2\tilde{q}_2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_2M_3$ + $ \phi_1q_1\tilde{q}_1$ + $ M_5\phi_1q_2\tilde{q}_2$ + $ M_6q_1\tilde{q}_2$ 0.6751 0.8593 0.7856 [X:[], M:[0.7632, 0.8553, 1.1447, 0.7632, 0.7632, 0.671], q:[0.8553, 0.3816], qb:[0.7632, 0.4737], phi:[0.3816]] [X:[], M:[[-2], [3], [-3], [-2], [-2], [-7]], q:[[3], [-1]], qb:[[-2], [4]], phi:[[-1]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_6$, $ M_1$, $ M_4$, $ M_5$, $ \phi_1^2$, $ M_2$, $ M_3$, $ \phi_1q_2^2$, $ \phi_1\tilde{q}_2^2$, $ M_6^2$, $ M_1M_6$, $ M_4M_6$, $ M_5M_6$, $ M_6\phi_1^2$, $ M_1^2$, $ M_1M_4$, $ M_4^2$, $ M_1M_5$, $ M_4M_5$, $ M_5^2$, $ M_2M_6$, $ M_1\phi_1^2$, $ M_4\phi_1^2$, $ M_5\phi_1^2$, $ \phi_1^4$, $ \phi_1q_2\tilde{q}_1$, $ M_1M_2$, $ M_2M_4$, $ M_2M_5$, $ M_2\phi_1^2$, $ \phi_1q_1q_2$, $ q_1\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_2^2$, $ \phi_1q_1\tilde{q}_2$, $ M_3M_6$, $ M_6\phi_1q_2^2$, $ M_1M_3$, $ M_3M_4$, $ M_3M_5$, $ M_3\phi_1^2$, $ M_4\phi_1q_2^2$, $ M_5\phi_1q_2^2$, $ \phi_1^3q_2^2$, $ \phi_1\tilde{q}_1^2$ $M_2\phi_1q_2^2$, $ M_6\phi_1\tilde{q}_2^2$ -2 t^2.01 + 4*t^2.29 + t^2.57 + 2*t^3.43 + t^3.99 + t^4.03 + 4*t^4.3 + 11*t^4.58 + 5*t^4.86 + t^5.13 + 2*t^5.45 + 6*t^5.72 - 2*t^6. + t^6.04 + 2*t^6.28 + 4*t^6.32 + t^6.55 + 11*t^6.59 + 26*t^6.87 + 9*t^7.14 + 2*t^7.46 - t^7.7 + 6*t^7.74 + t^7.97 + 10*t^8.01 + t^8.05 - 11*t^8.29 + 4*t^8.33 - 4*t^8.57 + 11*t^8.61 + t^8.84 + 26*t^8.88 - t^4.14/y - t^6.16/y - (4*t^6.43)/y + (4*t^7.3)/y + (7*t^7.58)/y + (8*t^7.86)/y + t^8.13/y - t^8.17/y - (2*t^8.45)/y - (2*t^8.72)/y - t^4.14*y - t^6.16*y - 4*t^6.43*y + 4*t^7.3*y + 7*t^7.58*y + 8*t^7.86*y + t^8.13*y - t^8.17*y - 2*t^8.45*y - 2*t^8.72*y t^2.01/g1^7 + (4*t^2.29)/g1^2 + g1^3*t^2.57 + (2*t^3.43)/g1^3 + g1^7*t^3.99 + t^4.03/g1^14 + (4*t^4.3)/g1^9 + (11*t^4.58)/g1^4 + 5*g1*t^4.86 + g1^6*t^5.13 + (2*t^5.45)/g1^10 + (6*t^5.72)/g1^5 - 2*t^6. + t^6.04/g1^21 + 2*g1^5*t^6.28 + (4*t^6.32)/g1^16 + g1^10*t^6.55 + (11*t^6.59)/g1^11 + (26*t^6.87)/g1^6 + (9*t^7.14)/g1 + (2*t^7.46)/g1^17 - g1^9*t^7.7 + (6*t^7.74)/g1^12 + g1^14*t^7.97 + (10*t^8.01)/g1^7 + t^8.05/g1^28 - (11*t^8.29)/g1^2 + (4*t^8.33)/g1^23 - 4*g1^3*t^8.57 + (11*t^8.61)/g1^18 + g1^8*t^8.84 + (26*t^8.88)/g1^13 - t^4.14/(g1*y) - t^6.16/(g1^8*y) - (4*t^6.43)/(g1^3*y) + (4*t^7.3)/(g1^9*y) + (7*t^7.58)/(g1^4*y) + (8*g1*t^7.86)/y + (g1^6*t^8.13)/y - t^8.17/(g1^15*y) - (2*t^8.45)/(g1^10*y) - (2*t^8.72)/(g1^5*y) - (t^4.14*y)/g1 - (t^6.16*y)/g1^8 - (4*t^6.43*y)/g1^3 + (4*t^7.3*y)/g1^9 + (7*t^7.58*y)/g1^4 + 8*g1*t^7.86*y + g1^6*t^8.13*y - (t^8.17*y)/g1^15 - (2*t^8.45*y)/g1^10 - (2*t^8.72*y)/g1^5


Deformation

Here is the data for the deformed fixed points from the chosen fixed point.

#SuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational
56267 $M_1q_1q_2$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ + $ M_2q_2\tilde{q}_1$ + $ M_3q_2\tilde{q}_2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_2M_3$ + $ \phi_1q_1\tilde{q}_1$ + $ M_5\phi_1q_2\tilde{q}_2$ + $ M_6q_1\tilde{q}_2$ + $ M_3M_7$ 0.6881 0.8804 0.7816 [X:[], M:[0.7692, 0.8461, 1.1539, 0.7692, 0.7692, 0.6924, 0.8461], q:[0.8461, 0.3846], qb:[0.7692, 0.4615], phi:[0.3846]] t^2.08 + 4*t^2.31 + 2*t^2.54 + t^3.46 + t^3.92 + t^4.15 + 4*t^4.38 + 12*t^4.62 + 9*t^4.85 + 3*t^5.08 + t^5.54 + 2*t^5.77 - 2*t^6. - t^4.15/y - t^4.15*y detail
56265 $M_1q_1q_2$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ + $ M_2q_2\tilde{q}_1$ + $ M_3q_2\tilde{q}_2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_2M_3$ + $ \phi_1q_1\tilde{q}_1$ + $ M_5\phi_1q_2\tilde{q}_2$ + $ M_6q_1\tilde{q}_2$ + $ M_6^2$ 0.6002 0.7609 0.7888 [X:[], M:[0.8571, 0.7143, 1.2857, 0.8571, 0.8571, 1.0], q:[0.7143, 0.4286], qb:[0.8571, 0.2857], phi:[0.4286]] t^2.14 + 4*t^2.57 + 2*t^3. + 2*t^3.86 + t^4.29 + 5*t^4.71 + 12*t^5.14 + 6*t^5.57 - t^4.29/y - t^4.29*y detail {a: 1647/2744, c: 261/343, M1: 6/7, M2: 5/7, M3: 9/7, M4: 6/7, M5: 6/7, M6: 1, q1: 5/7, q2: 3/7, qb1: 6/7, qb2: 2/7, phi1: 3/7}


Equivalent Fixed Points from Other Seed Theories

Here is a list of equivalent fixed points from other gauge theories.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore 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.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational
48181 SU2adj1nf2 $M_1q_1q_2$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ + $ M_2q_2\tilde{q}_1$ + $ M_3q_2\tilde{q}_2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_2M_3$ + $ \phi_1q_1\tilde{q}_1$ + $ M_5\phi_1q_2\tilde{q}_2$ 0.6542 0.8179 0.7999 [X:[], M:[0.7639, 0.8541, 1.1459, 0.7639, 0.7639], q:[0.8541, 0.382], qb:[0.7639, 0.4722], phi:[0.382]] 4*t^2.29 + t^2.56 + 2*t^3.44 + 2*t^3.98 + 10*t^4.58 + 5*t^4.85 + t^5.12 + 6*t^5.73 - 3*t^6. - t^4.15/y - t^4.15*y detail